Optical image capturing system

ABSTRACT

A six-piece optical lens for capturing image and a six-piece optical module for capturing image are provided. In order from an object side to an image side, the optical lens along the optical axis includes a first lens with refractive power, a second lens with refractive power, a third lens with refractive power, a fourth lens with refractive power, a fifth lens with refractive power and a sixth lens with refractive power. At least one of the image-side surface and object-side surface of each of the six lens elements is aspheric. The optical lens can increase aperture value and improve the imagining quality for use in compact cameras.

CROSS-REFERENCE TO RELATED APPLICATION

This application claims the benefit of Taiwan Patent Application No.104124440, filed on Jul. 28, 2015, in the Taiwan Intellectual PropertyOffice, the disclosure of which is incorporated herein in its entiretyby reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present disclosure relates to an optical image capturing system, andmore particularly to a compact optical image capturing system which canbe applied to electronic products.

2. Description of the Related Art

In recent years, with the rise of portable electronic devices havingcamera functionalities, the demand for an optical image capturing systemis raised gradually. The image sensing device of ordinary photographingcamera is commonly selected from charge coupled device (CCD) orcomplementary metal-oxide semiconductor sensor (CMOS Sensor). Inaddition, as advanced semiconductor manufacturing technology enables theminimization of pixel size of the image sensing device, the developmentof the optical image capturing system directs towards the field of highpixels. Therefore, the requirement for high imaging quality is rapidlyraised.

The traditional optical image capturing system of a portable electronicdevice comes with different designs, including a four-lens or afive-lens design. However, the requirement for the higher pixels and therequirement for a large aperture of an end user, like functionalities ofmicro filming and night view, or the requirement of wide view angle ofthe portable electronic device have been raised. But the optical imagecapturing system with the large aperture design often produces moreaberration resulting in the deterioration of quality in periphericalimage formation and difficulties of manufacturing, and the optical imagecapturing system with wide view angle design increases distortion ratein image formation, thus the optical image capturing system in priorarts cannot meet the requirement of the higher order camera lens module.

Therefore, how to effectively increase quantity of incoming light andview angle of the optical lenses, not only further improves total pixelsand imaging quality for the image formation, but also considers theequity design of the miniaturized optical lenses, becomes a quiteimportant issue.

SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an opticalimage capturing system and an optical image capturing lens which usecombination of refractive powers, convex and concave surfaces ofsix-piece optical lenses (the convex or concave surface in thedisclosure denotes the geometrical shape of an image-side surface or anobject-side surface of each lens on an optical axis) to increase thequantity of incoming light of the optical image capturing system and theview angle of the optical lenses, and to improve total pixels andimaging quality for image formation, so as to be applied to minimizedelectronic products.

The term and its definition to the lens element parameter in theembodiment of the present invention are shown as below for furtherreference.

The lens element parameter related to a length or a height in the lenselement

A maximum height for image formation of the optical image capturingsystem is denoted by HOI. A height of the optical image capturing systemis denoted by HOS. A distance from the object-side surface of the firstlens element to the image-side surface of the sixth lens element isdenoted by InTL. A distance from an aperture stop (aperture) to an imageplane is denoted by InS. A distance from the first lens element to thesecond lens element is denoted by In12 (instance). A central thicknessof the first lens element of the optical image capturing system on theoptical axis is denoted by TP (instance).

The lens element parameter related to a material in the lens element

An Abbe number of the first lens element in the optical image capturingsystem is denoted by NA1 (instance). A refractive index of the firstlens element is denoted by Nd1 (instance).

The lens element parameter related to a view angle in the lens element

A view angle is denoted by AF. Half of the view angle is denoted by HAF.A major light angle is denoted by MRA.

The lens element parameter related to exit/entrance pupil in the lenselement

An entrance pupil diameter of the optical image capturing system isdenoted by HEP. A maximum effective half diameter (EHD) of any surfaceof a single lens element refers to a perpendicular height between anintersection point on the surface of the lens element where the incidentlight with the maximum view angle in the optical system passes throughthe outmost edge of the entrance pupil and the optical axis. Forexample, the maximum effective half diameter of the object-side surfaceof the first lens element is denoted by EHD 11. The maximum effectivehalf diameter of the image-side surface of the first lens element isdenoted by EHD 12. The maximum effective half diameter of theobject-side surface of the second lens element is denoted by EHD 21. Themaximum effective half diameter of the image-side surface of the secondlens element is denoted by EHD 22. The maximum effective half diametersof any surfaces of other lens elements in the optical image capturingsystem are denoted in the similar way.

The lens element parameter related to a depth of the lens element shape

A distance in parallel with an optical axis from a maximum effectivediameter position to an axial point on the object-side surface of thesixth lens element is denoted by InRS61 (instance). A distance inparallel with an optical axis from a maximum effective diameter positionto an axial point on the image-side surface of the sixth lens element isdenoted by InRS62 (instance).

The lens element parameter related to the lens element shape

A critical point C is a tangent point on a surface of a specific lenselement, and the tangent point is tangent to a plane perpendicular tothe optical axis and the tangent point cannot be a crossover point onthe optical axis. To follow the past, a distance perpendicular to theoptical axis between a critical point C51 on the object-side surface ofthe fifth lens element and the optical axis is HVT51 (instance). Adistance perpendicular to the optical axis between a critical point C52on the image-side surface of the fifth lens element and the optical axisis HVT52 (instance). A distance perpendicular to the optical axisbetween a critical point C61 on the object-side surface of the sixthlens element and the optical axis is HVT61 (instance). A distanceperpendicular to the optical axis between a critical point C62 on theimage-side surface of the sixth lens element and the optical axis isHVT62 (instance). Distances perpendicular to the optical axis betweencritical points on the object-side surfaces or the image-side surfacesof other lens elements and the optical axis are denoted in the similarway described above.

The object-side surface of the sixth lens element has one inflectionpoint IF611 which is nearest to the optical axis, and the sinkage valueof the inflection point IF611 is denoted by SGI611 (instance). SGI611 isa horizontal shift distance in parallel with the optical axis from anaxial point on the object-side surface of the sixth lens element to theinflection point which is nearest to the optical axis on the object-sidesurface of the sixth lens element. A distance perpendicular to theoptical axis between the inflection point IF611 and the optical axis isHIF611 (instance). The image-side surface of the sixth lens element hasone inflection point IF621 which is nearest to the optical axis and thesinkage value of the inflection point IF621 is denoted by SGI621(instance). SGI621 is a horizontal shift distance in parallel with theoptical axis from an axial point on the image-side surface of the sixthlens element to the inflection point which is nearest to the opticalaxis on the image-side surface of the sixth lens element. A distanceperpendicular to the optical axis between the inflection point IF621 andthe optical axis is HIF621 (instance).

The object-side surface of the sixth lens element has one inflectionpoint IF612 which is the second nearest to the optical axis and thesinkage value of the inflection point IF612 is denoted by SGI612(instance). SGI612 is a horizontal shift distance in parallel with theoptical axis from an axial point on the object-side surface of the sixthlens element to the inflection point which is the second nearest to theoptical axis on the object-side surface of the sixth lens element. Adistance perpendicular to the optical axis between the inflection pointIF612 and the optical axis is HIF612 (instance). The image-side surfaceof the sixth lens element has one inflection point IF622 which is thesecond nearest to the optical axis and the sinkage value of theinflection point IF622 is denoted by SGI622 (instance). SGI622 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theinflection point which is the second nearest to the optical axis on theimage-side surface of the sixth lens element. A distance perpendicularto the optical axis between the inflection point IF622 and the opticalaxis is HIF622 (instance).

The object-side surface of the sixth lens element has one inflectionpoint IF613 which is the third nearest to the optical axis and thesinkage value of the inflection point IF613 is denoted by SGI613(instance). SGI613 is a horizontal shift distance in parallel with theoptical axis from an axial point on the object-side surface of the sixthlens element to the inflection point which is the third nearest to theoptical axis on the object-side surface of the sixth lens element. Adistance perpendicular to the optical axis between the inflection pointIF613 and the optical axis is HIF613 (instance). The image-side surfaceof the sixth lens element has one inflection point IF623 which is thethird nearest to the optical axis and the sinkage value of theinflection point IF623 is denoted by SGI623 (instance). SGI623 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theinflection point which is the third nearest to the optical axis on theimage-side surface of the sixth lens element. A distance perpendicularto the optical axis between the inflection point IF623 and the opticalaxis is HIF623 (instance).

The object-side surface of the sixth lens element has one inflectionpoint IF614 which is the fourth nearest to the optical axis and thesinkage value of the inflection point IF614 is denoted by SGI614(instance). SGI614 is a horizontal shift distance in parallel with theoptical axis from an axial point on the object-side surface of the sixthlens element to the inflection point which is the fourth nearest to theoptical axis on the object-side surface of the sixth lens element. Adistance perpendicular to the optical axis between the inflection pointIF614 and the optical axis is HIF614 (instance). The image-side surfaceof the sixth lens element has one inflection point IF624 which is thefourth nearest to the optical axis and the sinkage value of theinflection point IF624 is denoted by SGI624 (instance). SGI624 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theinflection point which is the fourth nearest to the optical axis on theimage-side surface of the sixth lens element. A distance perpendicularto the optical axis between the inflection point IF624 and the opticalaxis is HIF624 (instance).

The inflection points on the object-side surfaces or the image-sidesurfaces of the other lens elements and the distances perpendicular tothe optical axis thereof or the sinkage values thereof are denoted inthe similar way described above.

The lens element parameter related to an aberration

Optical distortion for image formation in the optical image capturingsystem is denoted by ODT. TV distortion for image formation in theoptical image capturing system is denoted by TDT. Further, the range ofthe aberration offset for the view of image formation may be limited to50%-100%. An offset of the spherical aberration is denoted by DFS. Anoffset of the coma aberration is denoted by DFC.

The vertical coordinate axis of the characteristic diagram of modulationtransfer function represents a contrast transfer rate (values are from 0to 1). The horizontal coordinate axis represents a spatial frequency(cycles/mm; lp/mm; line pairs per mm). Theoretically, an ideal imagecapturing system can 100% show the line contrast of a photographedobject. However, the values of the contrast transfer rate at thevertical coordinate axis are smaller than 1 in the actual imagecapturing system. The transfer rate of its comparison value is less thana vertical axis. In addition, comparing to the central region, it isgenerally more difficult to achieve a fine degree of recovery in theedge region of image capturing. The contrast transfer rates (MTF values)with spatial frequencies of 55 cycles/m at the optical axis, 0.3 fieldof view and 0.7 field of view of a visible spectrum on the image planeare respectively denoted by MTFE0, MTFE3 and MTFE7. The contrasttransfer rates (MTF values) with spatial frequencies of 110 cycles/m atthe optical axis, 0.3 field of view and 0.7 field of view on the imageplane are respectively denoted by MTFQ0, MTFQ3 and MTFQ7. The contrasttransfer rates (MTF values) with spatial frequencies of 220 cycles/m atthe optical axis, 0.3 field of view and 0.7 field of view on the imageplane are respectively denoted by MTFH0, MTFH3 and MTFH7. The contrasttransfer rates (MTF values) with spatial frequencies of 440 cycles/m atthe optical axis, 0.3 field of view and 0.7 field of view on the imageplane are respectively denoted by MTF0, MTF3 and MTF7. The three fieldsof view described above are representative to the centre, the internalfield of view and the external field of view of the lens elements. Thus,they may be used to evaluate whether the performance of a specificoptical image capturing system is excellent. The design of the opticalimage capturing system of the present invention mainly corresponds to apixel size in which a sensing device below 1.12 micrometers is includes.Therefore, the quarter spatial frequencies, the half spatial frequencies(half frequencies) and the full spatial frequencies (full frequencies)of the characteristic diagram of modulation transfer functionrespectively are at least 110 cycles/mm, 220 cycles/mm and 440cycles/mm.

If an optical image capturing system needs to satisfy with the imagesaimed to infrared spectrum, such as the requirement for night visionwith lower light source, the used wavelength may be 850 nm or 800 nm. Asthe main function is to recognize shape of an object formed inmonochrome and shade, the high resolution is unnecessary, and thus, aspatial frequency, which is less than 100 cycles/nun, is used toevaluate the functionality of the optical image capturing system, whenthe optical image capturing system is applied to the infrared spectrum.When the foregoing wavelength 850 nm is applied to focus on the imageplane, the contrast transfer rates (MTF values) with spatial frequenciesof 55 cycles/mm at the optical axis, 0.3 field of view and 0.7 field ofview on the image plane are respectively denoted by MTFI0, MTFI3 andMTFI7. However, the infrared wavelength of 850 nm or 800 nm may behugely different to wavelength of the regular visible light wavelength,and thus, it is hard to design an optical image capturing system whichhas to focus on the visible light and the infrared light (dual-mode)simultaneously while achieve a certain function respectively.

The disclosure provides an optical image capturing system, which is ableto focus on the visible light and the infrared light (dual-mode)simultaneously while achieve a certain function respectively, and anobject-side surface or an image-side surface of the fourth lens elementhas inflection points, such that the angle of incidence from each fieldof view to the fourth lens element can be adjusted effectively and theoptical distortion and the TV distortion can be corrected as well.Besides, the surfaces of the fourth lens element may have a betteroptical path adjusting ability to acquire better imaging quality.

The disclosure provides an optical image capturing system, in order froman object side to an image side, including a first, second, third,fourth, fifth, sixth lens elements and an image plane. The first lenselement has refractive power. An object-side surface and an image-sidesurface of the sixth lens element are aspheric. Focal lengths of thefirst through sixth lens elements are f1, f2, f3, f4, f5 and f6respectively. A focal length of the optical image capturing system is f.An entrance pupil diameter of the optical image capturing system is HEP.A distance from an object-side surface of the first lens element to theimage plane is HOS. Thicknesses in parallel with an optical axis of thefirst through sixth lens elements at height ½ HEP respectively are ETP1,ETP2, ETP3, ETP4, ETP5 and ETP6. A sum of ETP1 to ETP6 described aboveis SETP. Thicknesses of the first through sixth lens elements on theoptical axis respectively are TP1, TP2, TP3, TP4, TP5 and TP6. A sum ofTP1 to TP6 described above is STP. The following relations aresatisfied: 1.2≦f/HEP≦6.0 and 0.5≦SETP/STP<1.

The disclosure provides another optical image capturing system, in orderfrom an object side to an image side, including a first, second, third,fourth, fifth, sixth lens elements and an image plane. The first lenselement has refractive power and the position near the optical axis onan object-side surface of the first lens element may be a convexsurface. The second lens element has refractive power. The third lenselement has refractive power. The fourth lens element has refractivepower. The fifth lens element has positive refractive power. The sixthlens element has negative refractive power, and an object-side surfaceand an image-side surface of the sixth lens element are aspheric. Atleast two lens elements among the first through sixth lens elementsrespectively have at least one inflection point on at least one surfacethereof. At least one of the first through fourth lens elements haspositive refractive power. Focal lengths of the first through sixth lenselements are f1, f2, f3, f4, f5 and f6 respectively. A focal length ofthe optical image capturing system is f. An entrance pupil diameter ofthe optical image capturing system is HEP. A distance from anobject-side surface of the first lens element to the image plane is HOS.A horizontal distance in parallel with the optical axis from acoordinate point on the object-side surface of the first lens element atheight ½ HEP to the image plane is ETL. A horizontal distance inparallel with the optical axis from a coordinate point on theobject-side surface of the first lens element at height ½ HEP to acoordinate point on the image-side surface of the sixth lens element atheight ½ HEP is EIN. The following relations are satisfied:1.2≦f/HEP≦6.0 and 0.2≦EIN/ETL<1.

The disclosure provides another optical image capturing system, in orderfrom an object side to an image side, including a first, second, third,fourth, fifth, sixth lens elements and an image plane. The sixth lenselement has at least one inflection point on at least one surface amongan object-side surface and an image-side surface, wherein the opticalimage capturing system consists of six lens elements with refractivepower and at least three lens elements among the first through sixthlens elements respectively have at least one inflection point on atleast one surface thereof. The first lens element has refractive power.The second lens element has refractive power. The third lens element hasrefractive power. The fourth lens element has refractive power. Thefifth lens element has positive refractive power. The sixth lens elementhas negative refractive power. Focal lengths of the first through sixthlens elements are f1, f2, f3, f4, f5 and f6 respectively. A focal lengthof the optical image capturing system is f. An entrance pupil diameterof the optical image capturing system is HEP. A distance from anobject-side surface of the first lens element to the image plane is HOS.A horizontal distance in parallel with the optical axis from acoordinate point on the object-side surface of the first lens element atheight ½ HEP to the image plane is ETL. A horizontal distance inparallel with the optical axis from a coordinate point on theobject-side surface of the first lens element at height ½ HEP to acoordinate point on the image-side surface of the sixth lens element atheight ½ HEP is EIN. The following relations are satisfied:1.2≦f/HEP≦3.0 and 0.2≦EIN/ETL<1.

A thickness of a single lens element at height of ½ entrance pupildiameter (HEP) particularly affects the corrected aberration of commonarea of each field of view of light and the capability of correctingoptical path difference between each field of view of light in the scopeof ½ entrance pupil diameter (HEP). The capability of aberrationcorrection is enhanced if the thickness becomes greater, but thedifficulty for manufacturing is also increased at the same time.Therefore, it is necessary to control the thickness of a single lenselement at height of ½ entrance pupil diameter (HEP), in particular tocontrol the ratio relation (ETP/TP) of the thickness (ETP) of the lenselement at height of ½ entrance pupil diameter (HEP) to the thickness(TP) of the lens element to which the surface belongs on the opticalaxis. For example, the thickness of the first lens element at height of½ entrance pupil diameter (HEP) is denoted by ETP1. The thickness of thesecond lens element at height of ½ entrance pupil diameter (HEP) isdenoted by ETP2. The thicknesses of other lens elements are denoted inthe similar way. A sum of ETP1 to ETP6 described above is SETP. Theembodiments of the present invention may satisfy the following relation:0.3≦SETP/EIN<1.

In order to enhance the capability of aberration correction and reducethe difficulty for manufacturing at the same time, it is particularlynecessary to control the ratio relation (ETP/TP) of the thickness (ETP)of the lens element at height of ½ entrance pupil diameter (HEP) to thethickness (TP) of the lens element on the optical axis lens. Forexample, the thickness of the first lens element at height of ½ entrancepupil diameter (HEP) is denoted by ETP1. The thickness of the first lenselement on the optical axis is TP1. The ratio between both of them isETP1/TP1. The thickness of the second lens element at height of ½entrance pupil diameter (HEP) is denoted by ETP2. The thickness of thesecond lens element on the optical axis is TP2. The ratio between bothof them is ETP2/TP2. The ratio relations of the thicknesses of otherlens element in the optical image capturing system at height of ½entrance pupil diameter (HEP) to the thicknesses (TP) of the lenselements on the optical axis lens are denoted in the similar way. Theembodiments of the present invention may satisfy the following relation:0.2≦ETP/TP≦3.

A horizontal distance between two adjacent lens elements at height of ½entrance pupil diameter (HEP) is denoted by ED. The horizontal distance(ED) described above is in parallel with the optical axis of the opticalimage capturing system and particularly affects the corrected aberrationof common area of each field of view of light and the capability ofcorrecting optical path difference between each field of view of lightat the position of ½ entrance pupil diameter (HEP). The capability ofaberration correction may be enhanced if the horizontal distance becomesgreater, but the difficulty for manufacturing is also increased and thedegree of ‘miniaturization’ to the length of the optical image capturingsystem is restricted. Thus, it is essential to control the horizontaldistance (ED) between two specific adjacent lens elements at height of ½entrance pupil diameter (HEP).

In order to enhance the capability of aberration correction and reducethe difficulty for ‘miniaturization’ to the length of the optical imagecapturing system at the same time, it is particularly necessary tocontrol the ratio relation (ED/IN) of the horizontal distance (ED)between the two adjacent lens elements at height of ½ entrance pupildiameter (HEP) to the horizontal distance (IN) between the two adjacentlens elements on the optical axis. For example, the horizontal distancebetween the first lens element and the second lens element at height of½ entrance pupil diameter (HEP) is denoted by ED12. The horizontaldistance between the first lens element and the second lens element onthe optical axis is IN12. The ratio between both of them is ED12/IN12.The horizontal distance between the second lens element and the thirdlens element at height of ½ entrance pupil diameter (HEP) is denoted byED23. The horizontal distance between the second lens element and thethird lens element on the optical axis is IN23. The ratio between bothof them is ED23/IN23. The ratio relations of the horizontal distancesbetween other two adjacent lens elements in the optical image capturingsystem at height of ½ entrance pupil diameter (HEP) to the horizontaldistances between the two adjacent lens elements on the optical axis aredenoted in the similar way.

A horizontal distance in parallel with the optical axis from acoordinate point on the image-side surface of the sixth lens element atheight ½ HEP to the image plane is EBL. A horizontal distance inparallel with the optical axis from an axial point on the image-sidesurface of the sixth lens element to the image plane is BL. Theembodiments of the present invention enhance the capability ofaberration correction and reserve space for accommodating other opticalelements. The following relation may be satisfied: 0.2≦EBL/BL<1.1. Theoptical image capturing system may further include a light filtrationelement. The light filtration element is located between the sixth lenselement and the image plane. A distance in parallel with the opticalaxis from a coordinate point on the image-side surface of the sixth lenselement at height ½ HEP to the light filtration element is EIR. Adistance in parallel with the optical axis from an axial point on theimage-side surface of the sixth lens element to the light filtrationelement is PIR. The embodiments of the present invention may satisfy thefollowing relation: 0.1≦EIR/PIR≦1.1.

The height of optical system (HOS) may be reduced to achieve theminimization of the optical image capturing system when the absolutevalue of f1 is larger than f6 (|f1|>f6).

When |f2|+|f3|+|f4|+|f5| and |f1|+|f6| are satisfied with aboverelations, at least one of the second through fifth lens elements mayhave weak positive refractive power or weak negative refractive power.The weak refractive power indicates that an absolute value of the focallength of a specific lens element is greater than 10. When at least oneof the second through fifth lens elements has the weak positiverefractive power, the positive refractive power of the first lenselement can be shared, such that the unnecessary aberration will notappear too early. On the contrary, when at least one of the secondthrough fifth lens elements has the weak negative refractive power, theaberration of the optical image capturing system can be corrected andfine tuned.

The sixth lens element may have negative refractive power and a concaveimage-side surface. Hereby, the back focal length is reduced for keepingthe miniaturization, to miniaturize the lens element effectively. Inaddition, at least one of the object-side surface and the image-sidesurface of the sixth lens element may have at least one inflectionpoint, such that the angle of incident with incoming light from anoff-axis field of view can be suppressed effectively and the aberrationin the off-axis field of view can be corrected further.

BRIEF DESCRIPTION OF THE DRAWINGS

The detailed structure, operating principle and effects of the presentdisclosure will now be described in more details hereinafter withreference to the accompanying drawings that show various embodiments ofthe present disclosure as follows.

FIG. 1A is a schematic view of the optical image capturing systemaccording to the first embodiment of the present application.

FIG. 1B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the first embodimentof the present application.

FIG. 1C is a characteristic diagram of modulation transfer of a visiblelight according to the first embodiment of the present application.

FIG. 1D is a characteristic diagram of modulation transfer of infraredrays according to the first embodiment of the present application.

FIG. 2A is a schematic view of the optical image capturing systemaccording to the second embodiment of the present application.

FIG. 2B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the secondembodiment of the present application.

FIG. 2C is a characteristic diagram of modulation transfer of a visiblelight according to the second embodiment of the present application.

FIG. 2D is a characteristic diagram of modulation transfer of infraredrays according to the second embodiment of the present application.

FIG. 3A is a schematic view of the optical image capturing systemaccording to the third embodiment of the present application.

FIG. 3B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the third embodimentof the present application.

FIG. 3C is a characteristic diagram of modulation transfer of a visiblelight according to the third embodiment of the present application.

FIG. 3D is a characteristic diagram of modulation transfer of infraredrays according to the third embodiment of the present application.

FIG. 4A is a schematic view of the optical image capturing systemaccording to the fourth embodiment of the present application.

FIG. 4B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the fourthembodiment of the present application.

FIG. 4C is a characteristic diagram of modulation transfer of a visiblelight according to the fourth embodiment of the present application.

FIG. 4D is a characteristic diagram of modulation transfer of infraredrays according to the fourth embodiment of the present application.

FIG. 5A is a schematic view of the optical image capturing systemaccording to the fifth embodiment of the present application.

FIG. 5B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the fifth embodimentof the present application.

FIG. 5C is a characteristic diagram of modulation transfer of a visiblelight according to the fifth embodiment of the present application.

FIG. 5D is a characteristic diagram of modulation transfer of infraredrays according to the fifth embodiment of the present application.

FIG. 6A is a schematic view of the optical image capturing systemaccording to the sixth embodiment of the present application.

FIG. 6B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the sixth embodimentof the present application.

FIG. 6C is a characteristic diagram of modulation transfer of a visiblelight according to the sixth embodiment of the present application.

FIG. 6D is a characteristic diagram of modulation transfer of infraredrays according to the sixth embodiment of the present application.

FIG. 7A is a schematic view of the optical image capturing systemaccording to the seventh embodiment of the present application.

FIG. 7B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the seventhembodiment of the present application.

FIG. 7C is a characteristic diagram of modulation transfer of a visiblelight according to the seventh embodiment of the present application.

FIG. 7D is a characteristic diagram of modulation transfer of infraredrays according to the seventh embodiment of the present application.

FIG. 8A is a schematic view of the optical image capturing systemaccording to the eighth embodiment of the present application.

FIG. 8B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the eighthembodiment of the present application.

FIG. 8C is a characteristic diagram of modulation transfer of a visiblelight according to the eighth embodiment of the present application.

FIG. 8D is a characteristic diagram of modulation transfer of infraredrays according to the eighth embodiment of the present application.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Reference will now be made in detail to the exemplary embodiments of thepresent disclosure, examples of which are illustrated in theaccompanying drawings. Therefore, it is to be understood that theforegoing is illustrative of exemplary embodiments and is not to beconstrued as limited to the specific embodiments disclosed, and thatmodifications to the disclosed exemplary embodiments, as well as otherexemplary embodiments, are intended to be included within the scope ofthe appended claims. These embodiments are provided so that thisdisclosure will be thorough and complete, and will fully convey theinventive concept to those skilled in the art. The relative proportionsand ratios of elements in the drawings may be exaggerated or diminishedin size for the sake of clarity and convenience in the drawings, andsuch arbitrary proportions are only illustrative and not limiting in anyway. The same reference numbers are used in the drawings and thedescription to refer to the same or like parts.

It will be understood that, although the terms ‘first’, ‘second’,‘third’, etc., may be used herein to describe various elements, theseelements should not be limited by these terms. The terms are used onlyfor the purpose of distinguishing one component from another component.Thus, a first element discussed below could be termed a second elementwithout departing from the teachings of embodiments. As used herein, theterm “or” includes any and all combinations of one or more of theassociated listed items.

An optical image capturing system, in order from an object side to animage side, includes a first, second, third, fourth, fifth and sixthlens elements with refractive power and an image plane. The opticalimage capturing system may further include an image sensing device whichis disposed on an image plane.

The optical image capturing system may use three sets of wavelengthswhich are 486.1 nm, 587.5 nm and 656.2 nm, respectively, wherein 587.5nm is served as the primary reference wavelength and a referencewavelength for retrieving technical features. The optical imagecapturing system may also use five sets of wavelengths which are 470 nm,510 nm, 555 nm, 610 nm and 650 nm, respectively, wherein 555 nm isserved as the primary reference wavelength and a reference wavelengthfor retrieving technical features.

A ratio of the focal length f of the optical image capturing system to afocal length fp of each of lens elements with positive refractive poweris PPR. A ratio of the focal length f of the optical image capturingsystem to a focal length fn of each of lens elements with negativerefractive power is NPR. A sum of the PPR of all lens elements withpositive refractive power is ΣPPR. A sum of the NPR of all lens elementswith negative refractive powers is ΣNPR. It is beneficial to control thetotal refractive power and the total length of the optical imagecapturing system when following conditions are satisfied:0.5≦ΣPPR/ΣNPR|≦15. Preferably, the following relation may be satisfied:1≦ΣPPR/|ΣNPR|≦3.0.

The optical image capturing system may further include an image sensingdevice which is disposed on an image plane. Half of a diagonal of aneffective detection field of the image sensing device (imaging height orthe maximum image height of the optical image capturing system) is HOI.A distance on the optical axis from the object-side surface of the firstlens element to the image plane is HOS. The following relations aresatisfied: HOS/HOI≦10 and 0.5≦HOS/f≦10. Preferably, the followingrelations may be satisfied: 1≦HOS/HOI≦5 and 1≦HOS/f≦7. Hereby, theminiaturization of the optical image capturing system can be maintainedeffectively, so as to be carried by lightweight portable electronicdevices.

In addition, in the optical image capturing system of the disclosure,according to different requirements, at least one aperture stop may bearranged for reducing stray light and improving the imaging quality.

In the optical image capturing system of the disclosure, the aperturestop may be a front or middle aperture. The front aperture is theaperture stop between a photographed object and the first lens element.The middle aperture is the aperture stop between the first lens elementand the image plane. If the aperture stop is the front aperture, alonger distance between the exit pupil and the image plane of theoptical image capturing system can be formed, such that more opticalelements can be disposed in the optical image capturing system and theefficiency of receiving images of the image sensing device can beraised. If the aperture stop is the middle aperture, the view angle ofthe optical image capturing system can be expended, such that theoptical image capturing system has the same advantage that is owned bywide angle cameras. A distance from the aperture stop to the image planeis InS. The following relation is satisfied: 0.2≦InS/HOS≦1.1. Hereby,features of maintaining the minimization for the optical image capturingsystem and having wide-angle are available simultaneously.

In the optical image capturing system of the disclosure, a distance fromthe object-side surface of the first lens element to the image-sidesurface of the sixth lens element is InTL. A sum of central thicknessesof all lens elements with refractive power on the optical axis is ΣTP.The following relation is satisfied: 0.1≦ΣTP/InTL≦0.9. Hereby, contrastratio for the image formation in the optical image capturing system anddefect-free rate for manufacturing the lens element can be givenconsideration simultaneously, and a proper back focal length is providedto dispose other optical components in the optical image capturingsystem.

A curvature radius of the object-side surface of the first lens elementis R1. A curvature radius of the image-side surface of the first lenselement is R2. The following relation is satisfied: 0.001≦|R1/R2|≦20.Hereby, the first lens element may have proper strength of the positiverefractive power, so as to avoid the longitudinal spherical aberrationto increase too fast. Preferably, the following relation may besatisfied: 0.01≦|R1/R2|<10.

A curvature radius of the object-side surface of the sixth lens elementis R11. A curvature radius of the image-side surface of the sixth lenselement is R12. The following relation is satisfied:−7<(R11−R12)/(R11+R12)<50. Hereby, the astigmatism generated by theoptical image capturing system can be corrected beneficially.

A distance between the first lens element and the second lens element onthe optical axis is IN12. The following relation is satisfied:IN12/f≦3.0. Hereby, the chromatic aberration of the lens elements can beimproved, such that the performance can be increased.

A distance between the fifth lens element and the sixth lens element onthe optical axis is IN56. The following relation is satisfied:IN56/f≦0.8. Hereby, the chromatic aberration of the lens elements can beimproved, such that the performance can be increased.

Central thicknesses of the first lens element and the second lenselement on the optical axis are TP1 and TP2, respectively. The followingrelation is satisfied: 0.1≦(TP1+IN12)/TP2≦10. Hereby, the sensitivityproduced by the optical image capturing system can be controlled, andthe performance can be increased.

Central thicknesses of the fifth lens element and the sixth lens elementon the optical axis are TP5 and TP6, respectively, and a distancebetween the aforementioned two lens elements on the optical axis isIN56. The following relation is satisfied: 0.1≦(TP6+IN56)/TP5≦10.Hereby, the sensitivity produced by the optical image capturing systemcan be controlled and the total height of the optical image capturingsystem can be reduced.

Central thicknesses of the second lens element, the third lens elementand the fourth lens element on the optical axis are TP2. TP3 and TP4,respectively. A distance between the second lens element and the thirdlens element on the optical axis is IN23. A distance between the thirdlens element and the fourth lens element on the optical axis is IN34. Adistance between the fourth lens element and the fifth lens element onthe optical axis is IN45. A distance on the optical axis from theobject-side surface of the first lens element to the image-side surfaceof the sixth lens element is InTL The following relation is satisfied:0.1≦TP4/(IN34+TP4+IN45)<1. Hereby, the aberration generated by theprocess of moving the incident light can be adjusted slightly layer uponlayer, and the total height of the optical image capturing system can bereduced.

In the optical image capturing system of the disclosure, a distanceperpendicular to the optical axis between a critical point C61 on theobject-side surface of the sixth lens element and the optical axis isHVT61. A distance perpendicular to the optical axis between a criticalpoint C62 on the image-side surface of the sixth lens element and theoptical axis is HVT62. A horizontal displacement distance on the opticalaxis from an axial point on the object-side surface of the sixth lenselement to the critical point C61 is SGC61. A horizontal displacementdistance on the optical axis from an axial point on the image-sidesurface of the sixth lens element to the critical point C62 is SGC62.The following relations may be satisfied: 0 mm≦HVT61≦3 mm, 0 mm≦HVT62≦6mm, 0<HVT61/HVT62, 0 mm≦|SGC61|≦0.5 mm, 0 mm<|SGC62|≦2 mm and0<|SGC62|/(|SGC62|+TP6)≦0.9. Hereby, the aberration in the off-axis viewfield can be corrected.

The optical image capturing system of the disclosure satisfies thefollowing relation: 0.2≦HVT62/HOI≦0.9. Preferably, the followingrelation may be satisfied: 0.3≦HVT62/HOI≦0.8. Hereby, the aberration ofsurrounding view field can be corrected.

The optical image capturing system of the disclosure satisfies thefollowing relation: 0≦HVT62/HOS≦0.5. Preferably, the following relationmay be satisfied: 0.2≦HVT62/HOS≦0.45. Hereby, the aberration ofsurrounding view field can be corrected.

In the optical image capturing system of the disclosure, a distance inparallel with an optical axis from an inflection point on theobject-side surface of the sixth lens element which is nearest to theoptical axis to an axial point on the object-side surface of the sixthlens element is denoted by SGI611. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thesixth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the sixth lens element is denoted bySGI621. The following relations are satisfied: 0<SGI611/(SGI611+TP6)≦0.9and 0<SGI621/(SGI621+TP6)≦0.9. Preferably, the following relations maybe satisfied: 0.1≦SGI611/(SGI611+TP6)≦0.6 and0.1≦SGI621/(SGI621+TP6)≦0.6.

A distance in parallel with the optical axis from the inflection pointon the object-side surface of the sixth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the sixth lens element is denoted by SGI612. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the sixth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the sixth lenselement is denoted by SGI622. The following relations are satisfied:0<SGI612/(SGI612+TP6)≦0.9 and 0<SGI622/(SGI622+TP6)≦0.9. Preferably, thefollowing relations may be satisfied: 0.1≦SGI612/(SGI612+TP6)≦0.6 and0.1≦SGI622/(SGI622+TP6)≦0.6.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which isnearest to the optical axis and the optical axis is denoted by HIF611. Adistance perpendicular to the optical axis between an inflection pointon the image-side surface of the sixth lens element which is nearest tothe optical axis and an axial point on the image-side surface of thesixth lens element is denoted by HIF621. The following relations aresatisfied: 0.001 mm≦|HIF611|≦5 mm and 0.001 mm≦|HIF621|≦5 mm.Preferably, the following relations may be satisfied: 0.1mm≦|HIF611|≦3.5 mm and 1.5 mm≦|HIF621|≦3.5 mm.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF612. A distance perpendicular to the optical axis between an axialpoint on the image-side surface of the sixth lens element and aninflection point on the image-side surface of the sixth lens elementwhich is the second nearest to the optical axis is denoted by HIF622.The following relations are satisfied: 0.001 mm≦|HIF612|≦5 mm and 0.001mm≦|HIF622|≦5 nm. Preferably, the following relations may be satisfied:0.1 mm≦HIF622|≦3.5 mm and 0.1 mm≦|HIF612|≦3.5 mm.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thethird nearest to the optical axis and the optical axis is denoted byHIF613. A distance perpendicular to the optical axis between an axialpoint on the image-side surface of the sixth lens element and aninflection point on the image-side surface of the sixth lens elementwhich is the third nearest to the optical axis is denoted by HIF623. Thefollowing relations are satisfied: 0.001 mm≦|HIF613|≦5 mm and 0.001mm≦|HIF623|≦5 mm. Preferably, the following relations may be satisfied:0.1 mm≦|HIF623|≦3.5 mm and 0.1 mm≦|HIF613|≦3.5 mm.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thefourth nearest to the optical axis and the optical axis is denoted byHIF614. A distance perpendicular to the optical axis between an axialpoint on the image-side surface of the sixth lens element and aninflection point on the image-side surface of the sixth lens elementwhich is the fourth nearest to the optical axis is denoted by HIF624.The following relations are satisfied: 0.001 mm≦|HIF614|≦5 mm and 0.001mm≦|HIF624|≦5 mm. Preferably, the following relations may be satisfied:0.1 mm≦|HIF624|≦3.5 mm and 0.1 mm≦|HIF614|≦3.5 mm.

In one embodiment of the optical image capturing system of the presentdisclosure, the chromatic aberration of the optical image capturingsystem can be corrected by alternatively arranging the lens elementswith large Abbe number and small Abbe number.

The above Aspheric formula is:

z=ch ²/[1+[1−(k+1)c ² h ²]^(0.5) ]+A4h ⁴ +A6h ⁶ +A8h ⁸ +A10h ¹⁰ +A12h ¹²+A14h ¹⁴ +A16h ¹⁶ +A18h ¹⁸ +A20h ²⁰+ . . .   (1),

where z is a position value of the position along the optical axis andat the height h which reference to the surface apex; k is the coniccoefficient, c is the reciprocal of curvature radius, and A4, A6, A8,A10, A12, A14, A16, A18, and A20 are high order aspheric coefficients.

The optical image capturing system provided by the disclosure, the lenselements may be made of glass or plastic material. If plastic materialis adopted to produce the lens elements, the cost of manufacturing willbe lowered effectively. If lens elements are made of glass, the heateffect can be controlled and the designed space arranged for therefractive power of the optical image capturing system can be increased.Besides, the object-side surface and the image-side surface of the firstthrough sixth lens elements may be aspheric, so as to obtain morecontrol variables. Comparing with the usage of traditional lens elementmade by glass, the number of lens elements used can be reduced and theaberration can be eliminated. Thus, the total height of the opticalimage capturing system can be reduced effectively.

In addition, in the optical image capturing system provided by thedisclosure, if the lens element has a convex surface, the surface of thelens element adjacent to the optical axis is convex in principle. If thelens element has a concave surface, the surface of the lens elementadjacent to the optical axis is concave in principle.

The optical image capturing system of the disclosure can be adapted tothe optical image capturing system with automatic focus if required.With the features of a good aberration correction and a high quality ofimage formation, the optical image capturing system can be used invarious application fields.

The optical image capturing system of the disclosure can include adriving module according to the actual requirements. The driving modulemay be coupled with the lens elements to enable the lens elementsproducing displacement. The driving module may be the voice coil motor(VCM) which is applied to move the lens to focus, or may be the opticalimage stabilization (OIS) which is applied to reduce the distortionfrequency owing to the vibration of the lens while shooting.

At least one of the first, second, third, fourth, fifth and sixth lenselements of the optical image capturing system of the disclosure mayfurther be designed as a light filtration element with a wavelength lessthan 500 nm according to the actual requirement. The light filtrationelement may be made by coating at least one surface of the specific lenselement characterized of the filter function, and alternatively, may bemade by the lens element per se made of the material which is capable offiltering short wavelength.

According to the above embodiments, the specific embodiments withfigures are presented in detail as below.

The First Embodiment Embodiment 1

Please refer to FIG. 1A and FIG. 1B. FIG. 1A is a schematic view of theoptical image capturing system according to the first embodiment of thepresent application, FIG. 1B is longitudinal spherical aberrationcurves, astigmatic field curves, and an optical distortion curve of theoptical image capturing system in the order from left to right accordingto the first embodiment of the present application, FIG. 1C is acharacteristic diagram of modulation transfer of a visible lightaccording to the first embodiment of the present application, and FIG.1D is a characteristic diagram of modulation transfer of infrared raysaccording to the first embodiment of the present application. As shownin FIG. 1A, in order from an object side to an image side, the opticalimage capturing system includes a first lens element 110, an aperturestop 100, a second lens element 120, a third lens element 130, a fourthlens element 140, a fifth lens element 150, a sixth lens element 160, anIR-bandstop filter 180, an image plane 190, and an image sensing device192.

The first lens element 110 has negative refractive power and it is madeof plastic material. The first lens element 110 has a concaveobject-side surface 112 and a concave image-side surface 114, and bothof the object-side surface 112 and the image-side surface 114 areaspheric. The object-side surface 112 has two inflection points. Thethickness of the first lens element on the optical axis is TP1. Thethickness of the first lens element at height of ½ entrance pupildiameter (HEP) is denoted by ETP1.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the first lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefirst lens element is denoted by SGI111. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thefirst lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the first lens element is denoted bySGI121. The following relations are satisfied: SGI111=−0.0031 mm and|SGI111|/(SGI111|+TP1)=0.0016.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the first lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the first lens element is denoted by SGI112. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the first lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the first lenselement is denoted by SGI122. The following relations are satisfied:SGI112=1.3178 mm and |SGI112|/(|SGI112|+TP1)=0.4052.

A distance perpendicular to the optical axis from the inflection pointon the object-side surface of the first lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefirst lens element is denoted by HIF111. A distance perpendicular to theoptical axis from the inflection point on the image-side surface of thefirst lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the first lens element is denoted byHIF121. The following relations are satisfied: HIF111=0.5557 mm andHIF111/HOI=0.1111.

A distance perpendicular to the optical axis from the inflection pointon the object-side surface of the first lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the first lens element is denoted by HIF112. A distance perpendicularto the optical axis from the inflection point on the image-side surfaceof the first lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the first lenselement is denoted by HIF122. The following relations are satisfied:HIF112=5.3732 mm and HIF112/HOI=1.0746.

The second lens element 120 has positive refractive power and it is madeof plastic material. The second lens element 120 has a convexobject-side surface 122 and a convex image-side surface 124, and both ofthe object-side surface 122 and the image-side surface 124 are aspheric.The object-side surface 122 has an inflection point. The thickness ofthe second lens element on the optical axis is TP2. The thickness of thesecond lens element at height of ½ entrance pupil diameter (HEP) isdenoted by ETP2.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the second lens element which is nearest tothe optical axis to an axial point on the object-side surface of thesecond lens element is denoted by SGI211. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thesecond lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the second lens element is denoted bySGI221. The following relations are satisfied: SGI211=0.1069 mm,|SGI211|/(|SGI211|+TP2)=0.0412, SGI221=0 mm andSGI221|/(|SGI221|+TP2)=0.

A distance perpendicular to the optical axis from the inflection pointon the object-side surface of the second lens element which is nearestto the optical axis to an axial point on the object-side surface of thesecond lens element is denoted by HIF211. A distance perpendicular tothe optical axis from the inflection point on the image-side surface ofthe second lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the second lens element is denoted byHIF221. The following relations are satisfied: HIF211=1.1264 mm,HIF211/HOI=0.2253, HIF221=0 mm and HIF221/HOI=0.

The third lens element 130 has negative refractive power and it is madeof plastic material. The third lens element 130 has a concaveobject-side surface 132 and a convex image-side surface 134, and both ofthe object-side surface 132 and the image-side surface 134 are aspheric.The object-side surface 132 and the image-side surface 134 both have aninflection point. The thickness of the third lens element on the opticalaxis is TP3. The thickness of the third lens element at height of ½entrance pupil diameter (HEP) is denoted by ETP3.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the third lens element which is nearest tothe optical axis to an axial point on the object-side surface of thethird lens element is denoted by SGI311. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thethird lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the third lens element is denoted bySGI321. The following relations are satisfied: SGI311=−0.3041 mm,|SGI311|/(|SGI311|+TP3)=0.4445, SGI321=−0.1172 mm and|SGI321|/(|SGI321|+TP3)=0.2357.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the third lens element which isnearest to the optical axis and the optical axis is denoted by HIF311. Adistance perpendicular to the optical axis from the inflection point onthe image-side surface of the third lens element which is nearest to theoptical axis to an axial point on the image-side surface of the thirdlens element is denoted by HIF321. The following relations aresatisfied: HIF311=1.5907 mm, HIF311/HOI=0.3181, HIF321=1.3380 mm andHIF321/HOI=0.2676.

The fourth lens element 140 has positive refractive power and it is madeof plastic material. The fourth lens element 140 has a convexobject-side surface 142 and a concave image-side surface 144, and bothof the object-side surface 142 and the image-side surface 144 areaspheric. The object-side surface 142 has two inflection points and theimage-side surface 144 has an inflection point. The thickness of thefourth lens element on the optical axis is TP4. The thickness of thefourth lens element at height of ½ entrance pupil diameter (HEP) isdenoted by ETP4.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fourth lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefourth lens element is denoted by SGI411. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thefourth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the fourth lens element is denoted bySGI421. The following relations are satisfied: SGI411=0.0070 mm,|SGI411|/(|SGI411|+TP4)=0.0056, SGI421=0.0006 mm and|SGI421|/(|SGI421|+TP4)=0.0005.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fourth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the fourth lens element is denoted by SGI412. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fourth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the fourth lenselement is denoted by SGI422. The following relations are satisfied:SGI412=−0.2078 mm and |SGI412|/(|SGI412|+TP4)=0.1439.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fourth lens element which isnearest to the optical axis and the optical axis is denoted by HIF411. Adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the fourth lens element which is nearest tothe optical axis and the optical axis is denoted by HIF421. Thefollowing relations are satisfied: HIF411=0.4706 mm. HIF411/HOI=0.0941,HIF421=0.1721 mm and HIF421/HOI=0.0344.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fourth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF412. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fourth lens elementwhich is the second nearest to the optical axis and the optical axis isdenoted by HIF422. The following relations are satisfied: HIF412=2.0421mm and HIF412/HOI=0.4084.

The fifth lens element 150 has positive refractive power and it is madeof plastic material. The fifth lens element 150 has a convex object-sidesurface 152 and a convex image-side surface 154, and both of theobject-side surface 152 and the image-side surface 154 are aspheric. Theobject-side surface 152 has two inflection points and the image-sidesurface 154 has an inflection point. The thickness of the fifth lenselement on the optical axis is TP5. The thickness of the fifth lenselement at height of ½ entrance pupil diameter (HEP) is denoted by ETP5.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefifth lens element is denoted by SGI511. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thefifth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the fifth lens element is denoted bySGI521. The following relations are satisfied: SGI511=0.00364 mm,|SGI511|/(|SGI511|+TP5)=0.00338, SGI521=−0.63365 mm and|SGI521|/(|SGI521|+TP5)=0.37154.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the fifth lens element is denoted by SGI512. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fifth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the fifth lenselement is denoted by SGI522. The following relations are satisfied:SGI512=−0.32032 mm and |SGI512|/(|SGI512|+TP5)=0.23009.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is the thirdnearest to the optical axis to an axial point on the object-side surfaceof the fifth lens element is denoted by SGI513. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fifth lens element which is the third nearest to the optical axisto an axial point on the image-side surface of the fifth lens element isdenoted by SGI523. The following relations are satisfied: SGI513=0 mm,|SGI513|/(|SGI513|+TP5)=0, SGI523=0 mm and |SGI523|/(|SGI523|+TP5)=0.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is the fourthnearest to the optical axis to an axial point on the object-side surfaceof the fifth lens element is denoted by SGI514. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fifth lens element which is the fourth nearest to the opticalaxis to an axial point on the image-side surface of the fifth lenselement is denoted by SGI524. The following relations are satisfied:SGI514=0 mm, |SGI514|/(|SGI514|+TP5)=0, SGI524=0 mm and|SGI524|/(|SGI524|+TP5)=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which isnearest to the optical axis and the optical axis is denoted by HIF511. Adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the fifth lens element which is nearest tothe optical axis and the optical axis is denoted by HIF521. Thefollowing relations are satisfied: HIF511=0.28212 mm,HIF511/HOI=0.05642, HIF521=2.13850 mm and HIF521/HOI=0.42770.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF512. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fifth lens elementwhich is the second nearest to the optical axis and the optical axis isdenoted by HIF522. The following relations are satisfied: HIF512=2.51384mm and HIF512/HOI=0.50277.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which is thethird nearest to the optical axis and the optical axis is denoted byHIF513. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fifth lens elementwhich is the third nearest to the optical axis and the optical axis isdenoted by HIF523. The following relations are satisfied: HIF513=0 mm,HIF513/HOI=0, HIF523=0 mm and HIF523/HOI=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which is thefourth nearest to the optical axis and the optical axis is denoted byHIF514. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fifth lens elementwhich is the fourth nearest to the optical axis and the optical axis isdenoted by HIF524. The following relations are satisfied: HIF514=0 mm,HIF514/HOI=0, HIF524=0 mm and HIF524/HOI=0.

The sixth lens element 160 has negative refractive power and it is madeof plastic material. The sixth lens element 160 has a concaveobject-side surface 162 and a concave image-side surface 164, and theobject-side surface 162 has two inflection points and the image-sidesurface 164 has an inflection point. Hereby, the angle of incident ofeach view field on the sixth lens element can be effectively adjustedand the spherical aberration can thus be improved. The thickness of thesixth lens element on the optical axis is TP6. The thickness of thesixth lens element at height of ½ entrance pupil diameter (HEP) isdenoted by ETP6.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the sixth lens element which is nearest tothe optical axis to an axial point on the object-side surface of thesixth lens element is denoted by SGI611. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thesixth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the sixth lens element is denoted bySGI621. The following relations are satisfied: SGI611=−0.38558 mm,|SGI611|/(|SGI611|+TP6)=0.27212, SGI621=0.12386 mm and|SGI621|/(|SGI621|+TP6)=0.10722.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the sixth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the sixth lens element is denoted by SGI612. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the sixth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the sixth lenselement is denoted by SGI621. The following relations are satisfied:SGI612=−0.47400 mm, |SGI612|/(|SGI612|+TP6)=0.31488, SGI622=0 mm andSGI622|/(|SGI622|+TP6)=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which isnearest to the optical axis and the optical axis is denoted by HIF611. Adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the sixth lens element which is nearest tothe optical axis and the optical axis is denoted by HIF621. Thefollowing relations are satisfied: HIF611=2.24283 mm,HIF611/HOI=0.44857, HIF621=1.07376 mm and HIF621/HOI=0.21475.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF612. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the sixth lens elementwhich is the second nearest to the optical axis and the optical axis isdenoted by HIF622. The following relations are satisfied: HIF612=2.48895mm and HIF612/HOI=0.49779.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thethird nearest to the optical axis and the optical axis is denoted byHIF613. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the sixth lens elementwhich is the third nearest to the optical axis and the optical axis isdenoted by HIF623. The following relations are satisfied: HIF613=0 mm,HIF613/HOI=0, HIF623=0 mm and HIF623/HOI=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thefourth nearest to the optical axis and the optical axis is denoted byHIF614. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the sixth lens elementwhich is the fourth nearest to the optical axis and the optical axis isdenoted by HIF624. The following relations are satisfied: HIF614=0 mm,HIF614/HOI=0, HIF624=0 mm and HIF624/HOI=0.

In the first embodiment, a horizontal distance in parallel with theoptical axis from a coordinate point on the object-side surface of thefirst lens element at height ½ HEP to the image plane is ETL. Ahorizontal distance in parallel with the optical axis from a coordinatepoint on the object-side surface of the first lens element at height ½HEP to a coordinate point on the image-side surface of the sixth lenselement at height ½ HEP is EIN. The following relations are satisfied:ETL=19.304 mm, EIN=15.733 mm and EIN/ETL=0.815.

The first embodiment satisfies the following relations: ETP1=2.371 mm,ETP2=2.134 mm, ETP3=0.497 nmm, ETP4=1.111 mm, ETP5=1.783 mm andETP6=1.404 mm. A sum of ETP1 to ETP6 described above SETP=9.300 mm.TP1=2.064 mm, TP2=2.500 mm, TP3=0.380 mm, TP4=1.186 mm, TP5=2.184 mm andTP6=1.105 mm. A sum of TP1 to TP6 described above STP=9.419 mm.SETP/STP=0.987.

The present embodiment particularly controls the ratio relation (ETP/TP)of the thickness (ETP) of each lens element at height of ½ entrancepupil diameter (HEP) to the thickness (TP) of the lens element to whichthe surface belongs on the optical axis in order to achieve a balancebetween manufacturability and capability of aberration correction. Thefollowing relations are satisfied: ETP1/TP1=1.149, ETP2/TP2=0.854,ETP3/TP3=1.308, ETP4/TP4=0.936, ETP5/TP5=0.817 and ETP6/TP6=1.271.

The present embodiment controls a horizontal distance between each twoadjacent lens elements at height of ½ entrance pupil diameter (HEP) toachieve a balance between the degree of miniaturization for the lengthof the optical image capturing system HOS, the manufacturability and thecapability of aberration correction. The ratio relation (ED/IN) of thehorizontal distance (ED) between the two adjacent lens elements atheight of ½ entrance pupil diameter (HEP) to the horizontal distance(IN) between the two adjacent lens elements on the optical axis isparticularly controlled. The following relations are satisfied: ahorizontal distance in parallel with the optical axis between the firstlens element and the second lens element at height of ½ entrance pupildiameter (HEP) ED12=5.285 mm; a horizontal distance in parallel with theoptical axis between the second lens element and the third lens elementat height of ½ entrance pupil diameter (HEP) ED23=0.283 mm; a horizontaldistance in parallel with the optical axis between the third lenselement and the fourth lens element at height of ½ entrance pupildiameter (HEP) ED34=0.330 mm; a horizontal distance in parallel with theoptical axis between the fourth lens element and the fifth lens elementat height of ½ entrance pupil diameter (HEP) ED45=0.348 mm; a horizontaldistance in parallel with the optical axis between the fifth lenselement and the sixth lens element at height of ½ entrance pupildiameter (HEP) ED56=0.187 mm. A sum of ED12 to ED56 described above isdenoted as SED and SED=6.433 mm.

The horizontal distance between the first lens element and the secondlens element on the optical axis IN12=5.470 mm and ED12/IN12=0.966. Thehorizontal distance between the second lens element and the third lenselement on the optical axis IN23=0.178 mm and ED23/IN23=1.590. Thehorizontal distance between the third lens element and the fourth lenselement on the optical axis IN34=0.259 mm and ED34/IN34=1.273. Thehorizontal distance between the fourth lens element and the fifth lenselement on the optical axis IN45=0.209 mm and ED45/IN45=1.664. Thehorizontal distance between the fifth lens element and the sixth lenselement on the optical axis IN56=0.034 mm and ED56/IN56=5.557. A sum ofIN12 to IN56 described above is denoted as SIN. SIN=6.150 mm.SED/SIN=1.046.

The first embodiment also satisfies the following relations:ED12/ED23=18.685, ED23/ED34=0.857, ED34/ED45=0.947, ED45/ED56=1.859,IN12/IN23=30.746, IN23/IN34=0.686, IN34/IN45=1.239 and IN45/IN56=6.207.

A horizontal distance in parallel with the optical axis from acoordinate point on the image-side surface of the sixth lens element atheight ½ HEP to the image plane EBL=3.570 mm. A horizontal distance inparallel with the optical axis from an axial point on the image-sidesurface of the sixth lens element to the image plane BL=4.032 mm. Theembodiment of the present invention may satisfy the following relation:EBL/BL=0.8854. In the present invention, a distance in parallel with theoptical axis from a coordinate point on the image-side surface of thesixth lens element at height ½ HEP to the IR-bandstop filter EIR=1.950mm. A distance in parallel with the optical axis from an axial point onthe image-side surface of the sixth lens element to the IR-bandstopfilter PIR=2.121 mm. The following relation is satisfied: EIR/PIR=0.920.

The IR-bandstop filter 180 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 160 and the image plane 190.

In the optical image capturing system of the first embodiment, a focallength of the optical image capturing system is f, an entrance pupildiameter of the optical image capturing system is HEP, and half of amaximal view angle of the optical image capturing system is HAF. Thedetailed parameters are shown as below: f=4.075 mm, f/HEP=1.4,HAF=50.001′ and tan(HAF)=1.1918.

In the optical image capturing system of the first embodiment, a focallength of the first lens element 110 is f1 and a focal length of thesixth lens element 160 is f6. The following relations are satisfied:f1=−7.828 mm, |f/f1|=0.52060, f6=−4.886 and |f1|>|f6|.

In the optical image capturing system of the first embodiment, focallengths of the second lens element 120 to the fifth lens element 150 aref2, f3, f4 and f5, respectively. The following relations are satisfied:|f2|+|f3|+|f4|+|f5|=95.50815 mm, |f1|+|f6|=12.71352 mm and|f2|+|f3|+|f4|+|f5|>|f1|+|f6|.

A ratio of the focal length f of the optical image capturing system to afocal length fp of each of lens elements with positive refractive poweris PPR. A ratio of the focal length f of the optical image capturingsystem to a focal length fn of each of lens elements with negativerefractive power is NPR. In the optical image capturing system of thefirst embodiment, a sum of the PPR of all lens elements with positiverefractive power is ΣPPR=f/f1+f/f3+f/f5=1.63290. A sum of the NPR of alllens elements with negative refractive powers isΣNPR=f/f1|+|f/f3|+|f/f6|=1.51305, ΣPPR/|ΣNPR|=1.07921. The followingrelations are also satisfied: f/f2|=0.69101, |f/f3=0.15834,|f/f4|=0.06883, |f/f5|=0.87305 and |f/f6|=0.83412.

In the optical image capturing system of the first embodiment, adistance from the object-side surface 112 of the first lens element tothe image-side surface 164 of the sixth lens element is InTL. A distancefrom the object-side surface 112 of the first lens element to the imageplane 190 is HOS. A distance from an aperture 100 to an image plane 190is InS. Half of a diagonal length of an effective detection field of theimage sensing device 192 is HOI. A distance from the image-side surface164 of the sixth lens element to the image plane 190 is BFL. Thefollowing relations are satisfied: InTL+BFL=HOS, HOS=19.54120 mm,HOI=5.0 mm, HOS/HOI=3.90824, HOS/f=4.7952, InS=11.685 mm andInS/HOS=0.59794.

In the optical image capturing system of the first embodiment, a totalcentral thickness of all lens elements with refractive power on theoptical axis is ΣTP. The following relations are satisfied: ΣTP=8.13899mm and ΣTP/InTL=0.52477. Hereby, contrast ratio for the image formationin the optical image capturing system and defect-free rate formanufacturing the lens element can be given considerationsimultaneously, and a proper back focal length is provided to disposeother optical components in the optical image capturing system.

In the optical image capturing system of the first embodiment, acurvature radius of the object-side surface 112 of the first lenselement is R1. A curvature radius of the image-side surface 114 of thefirst lens element is R2. The following relation is satisfied:|R1/R2|=8.99987. Hereby, the first lens element may have proper strengthof the positive refractive power, so as to avoid the longitudinalspherical aberration to increase too fast.

In the optical image capturing system of the first embodiment, acurvature radius of the object-side surface 162 of the sixth lenselement is R11. A curvature radius of the image-side surface 164 of thesixth lens element is R12. The following relation is satisfied:(R11−R12)/(R11+R12)=1.27780. Hereby, the astigmatism generated by theoptical image capturing system can be corrected beneficially.

In the optical image capturing system of the first embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=f1+f3+f5=69.770 mm andf5/(f2+f4+f5)=0.067. Hereby, it is favorable for allocating the positiverefractive power of the first lens element 110 to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the first embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=f1+f3+f6=−38.451 mm andf6/(f1+f3+f6)=0.127. Hereby, it is favorable for allocating the positiverefractive power of the sixth lens element 160 to other negative lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the first embodiment, adistance between the first lens element 110 and the second lens element120 on the optical axis is IN12. The following relations are satisfied:IN12=6.418 mm and IN12/f=1.57491. Hereby, the chromatic aberration ofthe lens elements can be improved, such that the performance can beincreased.

In the optical image capturing system of the first embodiment, adistance between the fifth lens element 150 and the sixth lens element160 on the optical axis is IN56. The following relations are satisfied:IN56=0.025 mm and IN56/f=0.00613. Hereby, the chromatic aberration ofthe lens elements can be improved, such that the performance can beincreased.

In the optical image capturing system of the first embodiment, centralthicknesses of the first lens element 110 and the second lens element120 on the optical axis are TP1 and TP2, respectively. The followingrelations are satisfied: TP1=1.934 mm, TP2=2.486 mm and(TP1+IN12)/TP2=3.36005. Hereby, the sensitivity produced by the opticalimage capturing system can be controlled, and the performance can beincreased.

In the optical image capturing system of the first embodiment, centralthicknesses of the fifth lens element 150 and the sixth lens element 160on the optical axis are TP5 and TP6, respectively, and a distancebetween the aforementioned two lens elements on the optical axis isIN56. The following relations are satisfied: TP5=1.072 mm, TP6=1.031 mmand (TP6+IN56)/TP5=0.98555. Hereby, the sensitivity produced by theoptical image capturing system can be controlled and the total height ofthe optical image capturing system can be reduced.

In the optical image capturing system of the first embodiment, adistance between the third lens element 130 and the fourth lens element140 on the optical axis is IN34. A distance between the fourth lenselement 140 and the fifth lens element 150 on the optical axis is IN45.The following relations are satisfied: IN34=0.401 mm, IN45=0.025 nmm andTP4/(IN34+TP4+IN45)=0.74376. Hereby, the aberration generated by theprocess of moving the incident light can be adjusted slightly layer uponlayer, and the total height of the optical image capturing system can bereduced.

In the optical image capturing system of the first embodiment, adistance in parallel with an optical axis from a maximum effective halfdiameter position to an axial point on the object-side surface 152 ofthe fifth lens element is InRS51. A distance in parallel with an opticalaxis from a maximum effective half diameter position to an axial pointon the image-side surface 154 of the fifth lens element is InRS52. Acentral thickness of the fifth lens element 150 is TP5. The followingrelations are satisfied: InRS51=−0.34789 mm, InRS52=−0.88185 nmm,|InRS51|/TP5=0.32458 and |InRS52|/TP5=0.82276. Hereby, it is favorablefor manufacturing and forming the lens element and for maintaining theminimization for the optical image capturing system.

In the optical image capturing system of the first embodiment, adistance perpendicular to the optical axis between a critical point C51on the object-side surface 152 of the fifth lens element and the opticalaxis is HVT51. A distance perpendicular to the optical axis between acritical point C52 on the image-side surface 154 of the fifth lenselement and the optical axis is HVT52. The following relations aresatisfied: HVT51=0.515349 mm and HVT52=0 mm.

In the optical image capturing system of the first embodiment, adistance in parallel with an optical axis from a maximum effective halfdiameter position to an axial point on the object-side surface 162 ofthe sixth lens element is InRS61. A distance in parallel with an opticalaxis from a maximum effective half diameter position to an axial pointon the image-side surface 164 of the sixth lens element is InRS62. Acentral thickness of the sixth lens element 160 is TP6. The followingrelations are satisfied: InRS61=−0.58390 mm, InRS62=0.41976 mm,|InRS61|/TP6=0.56616 and |InRS62|/TP6|=0.40700. Hereby, it is favorablefor manufacturing and forming the lens element and for maintaining theminimization for the optical image capturing system.

In the optical image capturing system of the first embodiment, adistance perpendicular to the optical axis between a critical point C61on the object-side surface 162 of the sixth lens element and the opticalaxis is HVT61. A distance perpendicular to the optical axis between acritical point C62 on the image-side surface 164 of the sixth lenselement and the optical axis is HVT62. The following relations aresatisfied: HVT61=0 mm and HVT62=0 mm.

In the optical image capturing system of the first embodiment, thefollowing relation is satisfied: HVT51/HOI=0.1031. Hereby, theaberration of surrounding view field can be corrected.

In the optical image capturing system of the first embodiment, thefollowing relation is satisfied: HVT51/HOS=0.02634. Hereby, theaberration of surrounding view field can be corrected.

In the optical image capturing system of the first embodiment, thesecond lens element 120, the third lens element 130 and the sixth lenselement 160 have negative refractive power. An Abbe number of the secondlens element is NA2. An Abbe number of the third lens element is NA3. AnAbbe number of the sixth lens element is NA6. The following relation issatisfied: NA6/NA2≦1. Hereby, the chromatic aberration of the opticalimage capturing system can be corrected.

In the optical image capturing system of the first embodiment, TVdistortion and optical distortion for image formation in the opticalimage capturing system are TDT and ODT, respectively. The followingrelations are satisfied: |TDT|=2.124% and |ODT|=5.076%.

In the optical image capturing system of the present embodiment,contrast transfer rates of modulation transfer with spatial frequenciesof 55 cycles/mm of a visible light at the optical axis on the imageplane, 0.3 HOI and 0.7 HOI are respectively denoted by MTFE0, MTFE3 andMTFE7. The following relations are satisfied: MTFE0 is about 0.84, MTFE3is about 0.84 and MTFE7 is about 0.75. The contrast transfer rates ofmodulation transfer with spatial frequencies of 110 cycles/mm of avisible light at the optical axis on the image plane, 0.3 HOI and 0.7HOI are respectively denoted by MTFQ0, MTFQ3 and MTFQ7. The followingrelations are satisfied: MTFQ0 is about 0.66, MTFQ3 is about 0.65 andMTFQ7 is about 0.51. The contrast transfer rates of modulation transferwith spatial frequencies of 220 cycles/mm (MTF values) at the opticalaxis on the image plane, 0.3 HOI and 0.7 HOI are respectively denoted byMTFH0, MTFH3 and MTFH7. The following relations are satisfied: MTFH0 isabout 0.17, MTFH3 is about 0.07 and MTFH7 is about 0.14.

In the optical image capturing system of the present embodiment, whenthe infrared wavelength 850 nm is applied to focus on the image plane,contrast transfer rates of modulation transfer with a spatial frequency(55 cycles/mm) (MTF values) of the image at the optical axis on theimage plane, 0.3 HOI and 0.7 HOI are respectively denoted by MTFI0,MTFI3 and MTFI7. The following relations are satisfied: MTFI0 is about0.81, MTFI3 is about 0.8 and MTFI7 is about 0.15.

Please refer to the following Table 1 and Table 2.

The detailed data of the optical image capturing system of the firstembodiment is as shown in Table 1.

TABLE 1 Data of the optical image capturing system f = 4.075 mm, f/HEP =1.4, HAF = 50.000 deg Focal Surface # Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano Plano 1 Lens 1 −40.996257041.934 Plastic 1.515 56.55 −7.828 2 4.555209289 5.923 3 Ape. stop Plano0.495 4 Lens 2 5.333427366 2.486 Plastic 1.544 55.96 5.897 5−6.781659971 0.502 6 Lens 3 −5.697794287 0.380 Plastic 1.642 22.46−25.738 7 −8.883957518 0.401 8 Lens 4 13.19225664 1.236 Plastic 1.54455.96 59.205 9 21.55681832 0.025 10 Lens 5 8.987806345 1.072 Plastic1.515 56.55 4.668 11 −3.158875374 0.025 12 Lens 6 −29.46491425 1.031Plastic 1.642 22.46 −4.886 13 3.593484273 2.412 14 IR-bandstop Plano0.200 1.517 64.13 filter 15 Plano 1.420 16 Image plane Plano Referencewavelength (d-line) = 555 nm, shield position: clear aperture (CA) ofthe first plano = 5.800 mm; clear aperture (CA) of the third plano =1.570 mm; clear aperture (CA) of the fifth plano = 1.950 mmAs for the parameters of the aspheric surfaces of the first embodiment,reference is made to Table 2.

TABLE 2 Aspheric Coefficients Surface # 1 2 4 5 6 7 8 k 4.310876E+01−4.707622E+00 2.616025E+00 2.445397E+00 5.645686E+00 −2.117147E+01−5.287220E+00 A4 7.054243E−03 1.714312E−02 −8.377541E−03 −1.789549E−02−3.379055E−03 −1.370959E−02 −2.937377E−02 A6 −5.233264E−04 −1.502232E−04−1.838068E−03 −3.657520E−03 −1.225453E−03 6.250200E−03 2.743532E−03 A83.077890E−05 −1.359611E−04 1.233332E−03 −1.131622E−03 −5.979572E−03−5.854426E−03 −2.457574E−03 A10 −1.260650E−06 2.680747E−05 −2.390895E−031.390351E−03 4.556449E−03 4.049451E−03 1.874319E−03 A12 3.319093E−08−2.017491E−06 1.998555E−03 −4.152857E−04 −1.177175E−03 −1.314592E−03−6.013661E−04 A14 −5.051600E−10 6.604615E−08 −9.734019E−04 5.487286E−051.370522E−04 2.143097E−04 8.792480E−05 A16 3.380000E−12 −1.301630E−092.478373E−04 −2.919339E−06 −5.974015E−06 −1.399894E−05 −4.770527E−06Surface # 9 10 11 12 13 k 6.200000E+01 −2.114008E+01 −7.699904E+00−6.155476E+01 −3.120467E−01 A4 −1.359965E−01 −1.263831E−01 −1.927804E−02−2.492467E−02 −3.521844E−02 A6 6.628518E−02 6.965399E−02 2.478376E−03−1.835360E−03 5.629654E−03 A8 −2.129167E−02 −2.116027E−02 1.438785E−033.201343E−03 −5.466925E−04 A10 4.396344E−03 3.819371E−03 −7.013749E−04−8.990757E−04 2.231154E−05 A12 −5.542899E−04 −4.040283E−04 1.253214E−041.245343E−04 5.548990E−07 A14 3.768879E−05 2.280473E−05 −9.943196E−06−8.788363E−06 −9.396920E−08 A16 −1.052467E−06 −5.165452E−07 2.898397E−072.494302E−07 2.728360E−09

Table 1 is the detailed structure data to the first embodiment in FIG.1A, wherein the unit of the curvature radius, the thickness, thedistance, and the focal length is millimeters (mm). Surfaces 0-16illustrate the surfaces from the object side to the image plane in theoptical image capturing system. Table 2 is the aspheric coefficients ofthe first embodiment, wherein k is the conic coefficient in the asphericsurface formula, and A1-A20 are the first to the twentieth orderaspheric surface coefficient. Besides, the tables in the followingembodiments are referenced to the schematic view and the aberrationgraphs, respectively, and definitions of parameters in the tables areequal to those in the Table 1 and the Table 2, so the repetitiousdetails will not be given here.

The Second Embodiment Embodiment 2

Please refer to FIG. 2A, FIG. 2B, FIGS. 2C, and 2D. FIG. 2A is aschematic view of the optical image capturing system according to thesecond embodiment of the present application, FIG. 2B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the second embodiment of the presentapplication, FIG. 2C is a characteristic diagram of modulation transferof a visible light according to the second embodiment of the presentapplication, and FIG. 2D is a characteristic diagram of modulationtransfer of infrared rays according to the second embodiment of thepresent application. As shown in FIG. 2A, in order from an object sideto an image side, the optical image capturing system includes a firstlens element 210, a second lens element 220, an aperture stop 200, athird lens element 230, a fourth lens element 240, a fifth lens element250, a sixth lens element 260, an IR-bandstop filter 280, an image plane290, and an image sensing device 292.

The first lens element 210 has negative refractive power and it is madeof plastic material. The first lens element 210 has a concaveobject-side surface 212 and a concave image-side surface 214, and bothof the object-side surface 212 and the image-side surface 214 areaspheric. The object-side surface 212 has an inflection point.

The second lens element 220 has positive refractive power and it is madeof plastic material. The second lens element 220 has a concaveobject-side surface 222 and a convex image-side surface 224, and both ofthe object-side surface 222 and the image-side surface 224 are aspheric.

The third lens element 230 has positive refractive power and it is madeof plastic material. The third lens element 230 has a concaveobject-side surface 232 and a convex image-side surface 234, and both ofthe object-side surface 232 and the image-side surface 234 are aspheric.The object-side surface 232 has two inflection points and the image-sidesurface 234 has an inflection point.

The fourth lens element 240 has positive refractive power and it is madeof plastic material. The fourth lens element 240 has a convexobject-side surface 242 and a convex image-side surface 244, and both ofthe object-side surface 242 and the image-side surface 244 are aspheric.

The fifth lens element 250 has positive refractive power and it is madeof plastic material. The fifth lens element 250 has a convex object-sidesurface 252 and a convex image-side surface 254, and both of theobject-side surface 252 and the image-side surface 254 are aspheric. Theobject-side surface 252 has an inflection point.

The sixth lens element 260 has negative refractive power and it is madeof plastic material. The sixth lens element 260 has a concaveobject-side surface 262 and a concave image-side surface 264. Hereby,the back focal length is reduced to miniaturize the lens elementeffectively. In addition, the image-side surface 264 has an inflectionpoint, such that the angle of incident with incoming light from anoff-axis view field can be suppressed effectively and the aberration inthe off-axis view field can be corrected further.

The IR-bandstop filter 280 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 260 and the image plane 290.

In the optical image capturing system of the second embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=325.794 mm andf5/ΣPP=0.013. Hereby, it is favorable for allocating the positiverefractive power of the first lens element 210 to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the second embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−11.113 mm andf6/ΣNP=0.434. Hereby, it is favorable for allocating the negativerefractive power of the sixth lens element 260 to other negative lenselements.

Please refer to the following Table 3 and Table 4.

The detailed data of the optical image capturing system of the secondembodiment is as shown in Table 3.

TABLE 3 Data of the optical image capturing system f = 3.229 mm; f/HEP =1.62; HAF = 58.2 deg Focal Surface # Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Lens 1 −22.047091772.352 Plastic 1.544 55.96 −6.293 2 4.221520541 4.556 3 Lens 2−9.568444632 2.418 Plastic 1.584 29.88 20.172 4 −5.788891528 3.193 5Ape. stop Plano 0.218 6 Lens 3 −61.42146563 0.418 Plastic 1.642 22.46292.451 7 −46.50464967 0.053 8 Lens 4 5.142266258 1.749 Plastic 1.54455.96 8.781 9 −61.96712711 0.293 10 Lens 5 12.50784503 1.314 Plastic1.544 55.96 4.390 11 −2.853802442 0.114 12 Lens 6 −3.334889495 0.968Plastic 1.642 22.46 −4.821 13 54.46472893 3.358 14 IR-bandstop Plano0.194 1.517 64.13 filter 15 Plano 1.376 16 Image plane Plano 17Reference wavelength (d-line) = 555 nm, shield position: clear aperture(CA) of the fourth plano = 2.617 mm; clear aperture (CA) of the fifthplano = 1.591 mm; clear aperture (CA) of the ninth plano = 1.987 mmAs for the parameters of the aspheric surfaces of the second embodiment,reference is made to Table 4.

TABLE 4 Aspheric Coefficients Surface # 1 2 3 4 6 7 8 k 1.680710E+00−2.196824E−02 −7.724353E+00 −3.378479E−01 1.039737E−05 −5.732182E−06−1.123500E+00 A4 1.040829E−03 4.292393E−04 −5.789293E−03 −9.947234E−052.746907E−02 3.830452E−02 6.127360E−03 A6 4.231550E−06 −8.361862E−044.985718E−04 3.112656E−04 −1.945149E−03 −1.083749E−02 −1.307008E−02 A8−1.322185E−06 2.305005E−04 −1.147573E−04 −1.132982E−04 −5.587713E−03−2.683916E−03 5.766126E−03 A10 4.775265E−08 −3.193814E−05 2.408017E−053.168213E−05 4.869991E−03 6.425258E−03 −3.508967E−05 A12 −8.342800E−102.299418E−06 −2.743356E−06 −5.015661E−06 −1.962384E−03 −3.159527E−03−6.190943E−04 A14 7.390000E−12 −8.497019E−08 1.726297E−07 4.315420E−073.774632E−04 6.591661E−04 1.639538E−04 A16 −3.000000E−14 1.248930E−09−4.699280E−09 −1.547572E−08 −2.895684E−05 −5.185557E−05 −1.324749E−05Surface # 9 10 11 12 13 k −1.142687E−03 −7.528425E+00 −3.756848E−02−2.137275E−01 −1.091944E+00 A4 −5.157435E−02 −4.106303E−02 −1.515402E−02−2.412281E−02 −4.352989E−03 A6 5.985949E−03 8.734538E−04 3.488728E−024.219782E−02 9.061247E−03 A8 1.084898E−03 3.291099E−03 −1.930267E−02−2.342733E−02 −4.512285E−03 A10 −6.696081E−04 −1.066730E−03 5.188296E−036.136441E−03 1.245916E−03 A12 1.523253E−04 8.918724E−05 −7.037800E−04−7.187509E−04 −1.958966E−04 A14 −2.274639E−05 9.807721E−06 3.961331E−051.365095E−05 1.612323E−05 A16 1.894823E−06 −1.343610E−06 −1.635201E−072.553661E−06 −5.374168E−07

In the second embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 3 and Table 4.

Second embodiment (Primary reference wavelength = 587.5 nm) ETP1 ETP2ETP3 ETP4 ETP5 ETP6 2.493 2.389 0.421 1.601 1.137 1.130 ETP1/TP1ETP2/TP2 ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 1.060 0.988 1.007 0.9160.866 1.167 ETL EBL EIN EIR PIR EIN/ETL 22.596 4.918 17.678 3.348 3.3580.782 SETP/EIN EIR/PIR SETP STP SETP/STP BL 0.519 0.997 9.171 9.2190.995 4.928 ED12 ED23 ED34 ED45 ED56 EBL/BL 4.380 3.511 0.130 0.3470.137 0.99797 SED SIN SED/SIN 8.507 8.427 1.010 ED12/IN12 ED23/IN23ED34/IN34 ED45/IN45 ED56/IN56 0.961 1.030 2.451 1.186 1.201 |f/f1||f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.51317 0.16009 0.01104 0.367770.73559 0.66991 TP4/(IN34 + Σ PPR Σ NPR Σ PPR/|Σ NPR| IN12/f IN56/fTP4 + IN45) 1.26345 1.19412 1.05806 1.41070 0.03542 0.83471 |f1/f2||f2/f3| (TP1 + IN12)/TP2 (TP6 + IN56)/TP5 0.31196 0.06898 2.856230.82403 HOS InTL HOS/HOI InS/HOS ODT % TDT % 22.57460 17.64620 4.514920.44544 −3.99894 2.43070 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS0.711832 0 0.00000 0.00000 0.00000 0.00000 |InRS62|/ TP2/TP3 TP3/TP4InRS61 InRS62 |InRS61|/TP6 TP6 5.78289 0.23916 −0.70633 0.18152 0.729420.18746 MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.88 0.82 0.3 0.75 0.58 0.06MTFI0 MTFI3 MTFI7 0.85 0.77 0.45

The following contents may be deduced from Table 3 and Table 4.

Related inflection point values of second embodiment (Primary referencewavelength: 555 nm) HIF111 1.9679 HIF111/HOI 0.3936 SGI111 −0.0727|SGI111|/(|SGI111| + TP1) 0.0300 HIF311 0.2234 HIF311/HOI 0.0447 SGI311−0.0003 |SGI311|/(|SGI311| + TP3) 0.0008 HIF312 1.5312 HIF312/HOI 0.3062SGI312 0.0776 |SGI312|/(|SGI312| + TP3) 0.1565 HIF321 0.2202 HIF321/HOI0.0440 SGI321 −0.00043 |SGI321|/(|SGI321| + TP3) 0.0010 HIF511 0.4043HIF511/HOI 0.0809 SGI511 0.005433 |SGI511|/(|SGI511| + TP5) 0.0041HIF621 2.2697 HIF621/HOI 0.4539 SGI621 0.13745 |SGI621|/(|SGI621| + TP6)0.1243

The Third Embodiment Embodiment 3

Please refer to FIG. 3A, FIG. 3B, FIGS. 3C, and 3D. FIG. 3A is aschematic view of the optical image capturing system according to thethird embodiment of the present application, FIG. 3B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the third embodiment of the presentapplication, FIG. 3C is a characteristic diagram of modulation transferof a visible light according to the third embodiment of the presentapplication, and FIG. 3D is a characteristic diagram of modulationtransfer of infrared rays according to the third embodiment of thepresent application. As shown in FIG. 3A, in order from an object sideto an image side, the optical image capturing system includes a firstlens element 310, an aperture stop 300, a second lens element 320, athird lens element 330, a fourth lens element 340, a fifth lens element350, a sixth lens element 360, an IR-bandstop filter 380, an image plane390, and an image sensing device 392.

The first lens element 310 has positive refractive power and it is madeof plastic material. The first lens element 310 has a convex object-sidesurface 312 and a concave image-side surface 314, and both of theobject-side surface 312 and the image-side surface 314 are aspheric andhave an inflection point.

The second lens element 320 has positive refractive power and it is madeof plastic material. The second lens element 320 has a convexobject-side surface 322 and a convex image-side surface 324, and both ofthe object-side surface 322 and the image-side surface 324 are aspheric.The object-side surface 322 has an inflection point.

The third lens element 330 has negative refractive power and it is madeof plastic material. The third lens element 330 has a concaveobject-side surface 332 and a convex image-side surface 334, and both ofthe object-side surface 332 and the image-side surface 334 are aspheric.The object-side surface 332 has an inflection point.

The fourth lens element 340 has positive refractive power and it is madeof plastic material. The fourth lens element 340 has a concaveobject-side surface 342 and a convex image-side surface 344, and both ofthe object-side surface 342 and the image-side surface 344 are aspheric.The object-side surface 342 has two inflection points and the image-sidesurface 344 has an inflection point.

The fifth lens element 350 has positive refractive power and it is madeof plastic material. The fifth lens element 350 has a convex object-sidesurface 352 and a concave image-side surface 354, and both of theobject-side surface 352 and the image-side surface 354 are aspheric. Theobject-side surface 352 has two inflection points and the image-sidesurface 354 has an inflection point.

The sixth lens element 360 has negative refractive power and it is madeof plastic material. The sixth lens element 360 has a concaveobject-side surface 362 and a convex image-side surface 364. Hereby, theback focal length is reduced to miniaturize the lens elementeffectively. In addition, the object-side surface 362 has two inflectionpoints and the image-side surface 364 has four inflection points, suchthat the angle of incident with incoming light from an off-axis viewfield can be suppressed effectively and the aberration in the off-axisview field can be corrected further.

The IR-bandstop filter 380 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 360 and the image plane 390.

In the optical image capturing system of the third embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=33.752 nmm andf5/ΣPP=0.193. Hereby, it is favorable for allocating the positiverefractive power of the first lens element 310 to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the third embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−15.057 mm andf6/ΣNP=0.702. Hereby, it is favorable for allocating the negativerefractive power of the sixth lens element 360 to other negative lenselements.

Please refer to the following Table 5 and Table 6.

The detailed data of the optical image capturing system of the thirdembodiment is as shown in Table 5.

TABLE 5 Data of the optical image capturing system f = 4.255 mm; f/HEP =1.405; HAF = 50.001 deg Focal Surface # Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano At infinity 1 Lens 13.548301361 0.657 Plastic 1.625 25.41 9.956 2 7.424287246 0.315 3 Ape.Stop Plano 0.532 4 Lens 2 27.04014205 0.767 Plastic 1.544 55.66 12.417 5−8.952946557 0.321 6 Lens 3 −2.122445098 0.344 Plastic 1.516 56.44−4.480 7 −27.17021995 0.053 8 Lens 4 −12.81509732 0.578 Plastic 1.63623.44 4.852 9 −2.544440344 0.025 10 Lens 5 2.973941417 1.152 Plastic1.631 24.31 6.527 11 8.753387061 0.515 12 Lens 6 −4.16794985 0.310Plastic 1.642 22.49 −10.577 13 −10.95698982 0.059 14 IR-bandstop Plano0.200 1.517 64.13 filter 15 Plano 1.419 16 Image plane Plano Referencewavelength (d-line) = 555 nm, shield position: clear aperture (CA) ofthe fifth plano = 1.860 mm; clear aperture (CA) of the eleventh plano =3.600 mmAs for the parameters of the aspheric surfaces of the third embodiment,reference is made to Table 6.

TABLE 6 Aspheric Coefficients Surface # 1 2 4 5 6 7 8 k −1.257088E+002.057193E−05 0.000000E+00 8.159106E+00 −2.811065E−01 0.000000E+000.000000E+00 A4 −1.335975E−03 1.337021E−02 −4.680369E−02 −3.700466E−02−1.771002E−01 −5.750709E−01 −2.933459E−01 A6 1.737730E−02 −3.410428E−027.328850E−02 2.798111E−02 2.872882E−01 6.888923E−01 3.363326E−01 A8−1.976758E−02 4.358225E−02 −1.729661E−01 −3.179725E−02 −2.306575E−01−4.789580E−01 −2.270435E−01 A10 1.172867E−02 −3.006593E−02 1.961162E−011.540789E−02 1.159529E−01 2.033768E−01 8.377471E−02 A12 −3.475093E−031.070258E−02 −1.274347E−01 −3.245657E−03 −3.381851E−02 −5.142434E−02−1.668955E−02 A14 4.197994E−04 −2.036252E−03 4.271420E−02 1.931428E−045.191576E−03 7.069220E−03 1.698990E−03 A16 −1.214379E−05 1.743149E−04−5.832862E−03 1.221620E−05 −3.225925E−04 −4.032706E−04 −6.936909E−05Surface # 9 10 11 12 13 k −3.439997E−02 −1.456403E−01 −8.756131E+00−1.071602E−03 3.758590E−01 A4 2.088398E−02 −7.429493E−02 −9.472001E−02−4.257915E−02 3.605041E−02 A6 −2.621987E−02 2.378322E−02 3.251844E−022.274389E−02 −9.544607E−03 A8 1.951180E−02 −6.241339E−03 −5.288256E−03−5.201021E−03 1.224422E−03 A10 −1.100131E−02 1.081984E−03 4.169401E−046.726189E−04 −8.278198E−05 A12 3.464384E−03 −1.228816E−04 −1.614215E−05−4.963260E−05 2.452611E−06 A14 −5.105411E−04 7.085087E−06 3.820732E−071.958437E−06 −6.910000E−12 A16 2.818995E−05 −1.449058E−07 −9.225640E−09−3.217836E−08 −1.034440E−09

The presentation of the aspheric surface formula in the third embodimentis similar to that in the first embodiment. Besides, the definitions ofparameters in following tables are equal to those in the firstembodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 5 and Table 6.

Third embodiment (Primary reference wavelength: 555 nm) ETP1 ETP2 ETP3ETP4 ETP5 ETP6 0.499 0.660 0.451 0.469 0.930 0.566 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 0.760 0.861 1.313 0.811 0.807 1.825ETL EBL EIN EIR PIR EIN/ETL 6.959 1.687 5.272 0.068 0.059 0.758 SETP/EINEIR/PIR SETP STP SETP/STP BL 0.519 0.997 3.575 3.808 0.939 1.678 ED12ED23 ED34 ED45 ED56 EBL/BL 0.597 0.074 0.123 0.632 0.271 1.0054 SED SINSED/SIN 1.697 1.760 0.964 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45ED56/IN56 0.706 0.231 2.330 25.266 0.525 |f/f1| |f/f2| |f/f3| |f/f4||f/f5| |f/f6| 0.42742 0.34271 0.94978 0.87708 0.65200 0.40235TP4/(IN34 + Σ PPR Σ NPR Σ PPR/|Σ NPR| IN12/f IN56/f TP4 + IN45) 1.871781.77955 1.05183 0.19884 0.12105 0.88136 |f1/f2| |f2/f3| (TP1 + IN12)/TP2(TP6 + IN56)/TP5 0.80180 2.77141 1.95998 0.71601 HOS InTL HOS/HOIInS/HOS ODT % TDT % 7.24652 5.56873 1.44930 0.86591 4.01876 5.77333HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 2.01599 0.82247 0.000000.00000 0.00000 0.00000 |InRS61|/ |InRS62|/ TP2/TP3 TP3/TP4 InRS61InRS62 TP6 TP6 2.23182 0.59448 −1.07679 −0.61576 3.47352 1.98631 MTFE0MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.33 0.14 0.08 0.18 0.05 0.07 MTFI0 MTFI3MTFI7 0.45 0.03 0.23

The following contents may be deduced from Table 5 and Table 6.

Related inflection point values of third embodiment (Primary referencewavelength: 555 nm) HIF111 1.6401 HIF111/HOI 0.3280 SGI111 0.4003|SGI111|/(|SGI111| + TP1) 0.3786 HIF121 1.2908 HIF121/HOI 0.2582 SGI1210.1128 |SGI121|/(|SGI121| + TP1) 0.1465 HIF211 0.4024 HIF211/HOI 0.0805SGI211 0.0026 |SGI211|/(|SGI211| + TP2) 0.0034 HIF311 1.3690 HIF311/HOI0.2738 SGI311 −0.45529 |SGI311|/(|SGI311| + TP3) 0.5698 HIF411 1.7113HIF411/HOI 0.3423 SGI411 −0.51508 |SGI411|/(|SGI411| + TP4) 0.4712HIF412 2.1098 HIF412/HOI 0.4220 SGI412 −0.7909 |SGI412|/(|SGI412| + TP4)0.5777 HIF421 1.7583 HIF421/HOI 0.3517 SGI421 −0.7042|SGI421|/(|SGI421| + TP4) 0.5492 HIF511 0.9321 HIF511/HOI 0.1864 SGI5110.1171 |SGI511|/(|SGI511| + TP5) 0.0923 HIF512 2.8499 HIF512/HOI 0.5700SGI512 −0.3355 |SGI512|/(|SGI512| + TP5) 0.2255 HIF521 0.4502 HIF521/HOI0.0900 SGI521 0.009526 |SGI521|/(|SGI521| + TP5) 0.0082 HIF611 2.1136HIF611/HOI 0.4227 SGI611 −0.58593 |SGI611|/(|SGI611| + TP6) 0.6540HIF612 3.7199 HIF612/HOI 0.7440 SGI612 −1.06933 |SGI612|/(|SGI612| +TP6) 0.7753 HIF621 0.5034 HIF621/HOI 0.1007 SGI621 −0.00941|SGI621|/(|SGI621| + TP6) 0.0295 HIF622 1.6409 HIF622/HOI 0.3282 SGI6220.002082 |SGI622|/(|SGI622| + TP6) 0.0067 HIF623 3.7997 HIF623/HOI0.7599 SGI623 −0.3758 |SGI623|/(|SGI623| + TP6) 0.5480 HIF624 4.0185HIF624/HOI 0.8037 SGI624 −0.5037 |SGI624|/(|SGI624| + TP6) 0.6190

The Fourth Embodiment Embodiment 4

Please refer to FIG. 4A, FIG. 4B, FIGS. 4C, and 4D. FIG. 4A is aschematic view of the optical image capturing system according to thefourth embodiment of the present application, FIG. 4B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the fourth embodiment of the presentapplication, FIG. 4C is a characteristic diagram of modulation transferof a visible light according to the fourth embodiment of the presentapplication, and FIG. 4D is a characteristic diagram of modulationtransfer of infrared rays according to the fourth embodiment of thepresent application. As shown in FIG. 4A, in order from an object sideto an image side, the optical image capturing system includes a firstlens element 410, an aperture stop 400, a second lens element 420, athird lens element 430, a fourth lens element 440, a fifth lens element450, a sixth lens element 460, an IR-bandstop filter 480, an image plane490, and an image sensing device 492.

The first lens element 410 has positive refractive power and it is madeof plastic material. The first lens element 410 has a convex object-sidesurface 412 and a concave image-side surface 414, and both of theobject-side surface 412 and the image-side surface 414 are aspheric andhave an inflection point.

The second lens element 420 has positive refractive power and it is madeof plastic material. The second lens element 420 has a convexobject-side surface 422 and a convex image-side surface 424, and both ofthe object-side surface 422 and the image-side surface 424 are aspheric.The object-side surface 422 has an inflection point.

The third lens element 430 has negative refractive power and it is madeof plastic material. The third lens element 430 has a concaveobject-side surface 432 and a convex image-side surface 434, and both ofthe object-side surface 432 and the image-side surface 434 are asphericand have an inflection point.

The fourth lens element 440 has positive refractive power and it is madeof plastic material. The fourth lens element 440 has a concaveobject-side surface 442 and a convex image-side surface 444, and both ofthe object-side surface 442 and the image-side surface 444 are asphericand have an inflection point.

The fifth lens element 450 has positive refractive power and it is madeof plastic material. The fifth lens element 450 has a convex object-sidesurface 452 and a concave image-side surface 454, and both of theobject-side surface 452 and the image-side surface 454 are aspheric. Theobject-side surface 452 has two inflection points and the image-sidesurface 454 has three inflection points.

The sixth lens element 460 has negative refractive power and it is madeof plastic material. The sixth lens element 460 has a concaveobject-side surface 462 and a convex image-side surface 464. Hereby, theback focal length is reduced to miniaturize the lens elementeffectively. In addition, the object-side surface 462 and the image-sidesurface 464 both have two inflection points, such that the angle ofincident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 480 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 460 and the image plane 490.

In the optical image capturing system of the fourth embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=32.512 mm and f5/ΣPP=0.20.Hereby, it is favorable for allocating the positive refractive power ofthe first lens element 410 to other positive lens elements and thesignificant aberrations generated in the process of moving the incidentlight can be suppressed.

In the optical image capturing system of the fourth embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−15.121 mm andf6/ΣNP=0.687. Hereby, it is favorable for allocating the negativerefractive power of the sixth lens element 460 to other negative lenselements.

Please refer to the following Table 7 and Table 8.

The detailed data of the optical image capturing system of the fourthembodiment is as shown in Table 7.

TABLE 7 Data of the optical image capturing system f = 4.241 mm; f/HEP =1.6; HAF = 50 deg Focal Surface# Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Lens 1 3.3638590860.631 Plastic 1.625 25.41 10.439 2 6.398611078 0.292 3 Ape. Stop Plano0.446 4 Lens 2 190.8456602 0.731 Plastic 1.544 55.66 10.021 5−5.626458734 0.403 6 Lens 3 −1.982628147 0.325 Plastic 1.516 56.44−4.732 7 −10.97624465 0.143 8 Lens 4 −7.321646538 0.563 Plastic 1.63623.44 5.540 9 −2.465393481 0.025 10 Lens 5 2.78013764 1.084 Plastic1.631 24.31 6.512 11 7.185115558 0.587 12 Lens 6 −4.142287373 0.311Plastic 1.642 22.49 −10.389 13 −11.103195 0.050 14 IR-band Plano 0.2001.517 64.13 stop filter 15 Plano 1.417 16 Image Plano plane Referencewavelength (d-line) = 555 nm, shield position: clear aperture (CA) ofthe fifth plano = 1.860 mm; clear aperture (CA) of the eleventh plano =3.60 mmAs for the parameters of the aspheric surfaces of the fourth embodiment,reference is made to Table 8.

TABLE 8 Aspheric Coefficients Surface # 1 2 4 5 6 7 8 k −1.257088E+002.057193E−05 0.000000E+00 8.159106E+00 −2.811065E−01 0.000000E+000.000000E+00 A4 −1.335975E−03 1.337021E−02 −4.680369E−02 −3.700466E−02−1.771002E−01 −5.750709E−01 −2.933459E−01 A6 1.737730E−02 −3.410428E−027.328850E−02 2.798111E−02 2.872882E−01 6.888923E−01 3.363326E−01 A8−1.976758E−02 4.358225E−02 −1.729661E−01 −3.179725E−02 −2.306575E−01−4.789580E−01 −2.270435E−01 A10 1.172867E−02 −3.006593E−02 1.961162E−011.540789E−02 1.159529E−01 2.033768E−01 8.377471E−02 A12 −3.475093E−031.070258E−02 −1.274347E−01 −3.245657E−03 −3.381851E−02 −5.142434E−02−1.668955E−02 A14 4.197994E−04 −2.036252E−03 4.271420E−02 1.931428E−045.191576E−03 7.069220E−03 1.698990E−03 A16 −1.214379E−05 1.743149E−04−5.832862E−03 1.221620E−05 −3.225925E−04 −4.032706E−04 −6.936909E−05Surface # 9 10 11 12 13 k −3.439997E−02 −1.456403E−01 −8.756131E+00−1.071602E−03 3.758590E−01 A4 2.088398E−02 −7.429493E−02 −9.472001E−02−4.257915E−02 3.605041E−02 A6 −2.621987E−02 2.378322E−02 3.251844E−022.274389E−02 −9.544607E−03 A8 1.951180E−02 −6.241339E−03 −5.288256E−03−5.201021E−03 1.224422E−03 A10 −1.100131E−02 1.081984E−03 4.169401E−046.726189E−04 −8.278198E−05 A12 3.464384E−03 −1.228816E−04 −1.614215E−05−4.963260E−05 2.452611E−06 A14 −5.105411E−04 7.085087E−06 3.820732E−071.958437E−06 −6.910000E−12 A16 2.818995E−05 −1.449058E−07 −9.225640E−09−3.217836E−08 −1.034440E−09

The presentation of the aspheric surface formula in the fourthembodiment is similar to that in the first embodiment. Besides thedefinitions of parameters in following tables are equal to those in thefirst embodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 7 and Table 8.

Fourth embodiment (Primary reference wavelength: 587.5 nm) ETP1 ETP2ETP3 ETP4 ETP5 ETP6 0.517 0.625 0.362 0.547 0.888 0.521 ETP1/TP1ETP2/TP2 ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 0.819 0.854 1.114 0.9720.819 1.674 ETL EBL EIN EIR PIR EIN/ETL 6.978 1.680 5.298 0.064 0.0500.759 SETP/EIN EIR/PIR SETP STP SETP/STP BL 0.653 1.271 3.459 3.6450.949 1.666 ED12 ED23 ED34 ED45 ED56 EBL/BL 0.514 0.192 0.232 0.5100.391 1.0084 SED SIN SED/SIN 1.839 1.897 0.970 ED12/IN12 ED23/IN23ED34/IN34 ED45/IN45 ED56/IN56 0.696 0.477 1.620 20.389 0.666 |f/f1||f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.40625 0.42318 0.89622 0.765520.65124 0.40821 TP4/(IN34 + Σ PPR Σ NPR Σ PPR/|Σ NPR| IN12/f IN56/fTP4 + IN45) 1.97064 1.57997 1.24727 0.17417 0.13847 0.77007 |f1/f2||f2/f3| (TP1 + IN12)/TP2 (TP6 + IN56)/TP5 1.04169 2.11780 1.872380.82885 HOS InTL HOS/HOI InS/HOS ODT % TDT % 7.20808 5.54174 1.441620.87192 4.04571 5.62837 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS2.02646 0.67088 0.00000 0.00000 0.00000 0.00000 |InRS61|/ |InRS62|/TP2/TP3 TP3/TP4 InRS61 InRS62 TP6 TP6 2.25040 0.57748 −1.10342 −0.703393.54651 2.26076 MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.27 0.14 0.09 0.150.07 0.07 MTFI0 MTFI3 MTFI7 0.43 0.05 0.18

The following contents may be deduced from Table 7 and Table 8.

Related inflection point values of fourth embodiment (Primary referencewavelength: 555 nm) HIF111 1.4832 HIF111/HOI 0.2966 SGI111 0.346995|SGI111|/(|SGI111| + TP1) 0.3549 HIF121 1.1372 HIF121/HOI 0.2274 SGI1210.1027 |SGI121|/(|SGI121| + TP1) 0.1401 HIF211 0.0984 HIF211/HOI 0.0197SGI211 0.000021 |SGI211|/(|SGI211| + TP2) 0.00003 HIF311 1.1531HIF311/HOI 0.2306 SGI311 −0.3874 |SGI311|/(|SGI311| + TP3) 0.5438 HIF3211.6593 HIF321/HOI 0.3319 SGI321 −0.7072 |SGI321|/(|SGI321| + TP3) 0.6852HIF411 1.5572 HIF411/HOI 0.3114 SGI411 −0.5615 |SGI411|/(|SGI411| + TP4)0.4994 HIF421 1.7185 HIF421/HOI 0.3437 SGI421 −0.71215|SGI421|/(|SGI421| + TP4) 0.5586 HIF511 0.9366 HIF511/HOI 0.1873 SGI5110.117493 |SGI511|/(|SGI511| + TP5) 0.0978 HIF512 2.8110 HIF512/HOI0.5622 SGI512 −0.2957 |SGI512|/(|SGI512| + TP5) 0.2144 HIF521 0.3654HIF521/HOI 0.0731 SGI521 0.007632 |SGI521|/(|SGI521| + TP5) 0.0070HIF522 1.6107 HIF522/HOI 0.3221 SGI522 −0.0992 |SGI522|/(|SGI522| + TP5)0.0838 HIF523 1.8238 HIF523/HOI 0.3648 SGI523 −0.1410|SGI523|/(|SGI523| + TP5) 0.1151 HIF611 2.1056 HIF611/HOI 0.4211 SGI611−0.60304 |SGI611|/(|SGI611| + TP6) 0.6597 HIF612 3.4653 HIF612/HOI0.6931 SGI612 −1.0435 |SGI612|/(|SGI612| + TP6) 0.7703 HIF621 0.4970HIF621/HOI 0.0994 SGI621 −0.00907 |SGI621|/(|SGI621| + TP6) 0.0283HIF622 1.6069 HIF622/HOI 0.3214 SGI622 0.004565 |SGI622|/(|SGI622| +TP6) 0.0145

The Fifth Embodiment Embodiment 5

Please refer to FIG. 5A, FIG. 5B, FIGS. 5C, and 5D. FIG. 5A is aschematic view of the optical image capturing system according to thefifths embodiment of the present application, FIG. 5B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the fifth embodiment of the presentapplication, FIG. 5C is a characteristic diagram of modulation transferof a visible light according to the fifth embodiment of the presentapplication and FIG. 5D is a characteristic diagram of modulationtransfer of infrared rays according to the fifth embodiment of thepresent application. As shown in FIG. 5A, in order from an object sideto an image side, the optical image capturing system includes anaperture stop 500, a first lens element 510, a second lens element 520,a third lens element 530, a fourth lens element 540, a fifth lenselement 550, a sixth lens element 560, an IR-bandstop filter 580, animage plane 590, and an Image sensing device 592.

The first lens element 510 has positive refractive power and it is madeof plastic material. The first lens element 510 has a convex object-sidesurface 512 and a concave image-side surface 514, and both of theobject-side surface 512 and the image-side surface 514 are aspheric andhave an inflection point.

The second lens element 520 has positive refractive power and it is madeof plastic material. The second lens element 520 has a convexobject-side surface 522 and a convex image-side surface 524, and both ofthe object-side surface 522 and the image-side surface 524 are aspheric.The object-side surface 522 has an inflection point.

The third lens element 530 has negative refractive power and it is madeof plastic material. The third lens element 530 has a concaveobject-side surface 532 and a convex image-side surface 534, and both ofthe object-side surface 532 and the image-side surface 534 are aspheric.The object-side surface 532 has an inflection point and the image-sidesurface 534 has two inflection points.

The fourth lens element 540 has positive refractive power and it is madeof plastic material. The fourth lens element 540 has a concaveobject-side surface 542 and a convex image-side surface 544, and both ofthe object-side surface 542 and the image-side surface 544 are aspheric.The object-side surface 542 has three inflection points and theimage-side surface 544 has an inflection point.

The fifth lens element 550 has positive refractive power and it is madeof plastic material. The fifth lens element 550 has a convex object-sidesurface 552 and a concave image-side surface 554, and both of theobject-side surface 552 and the image-side surface 554 are aspheric andhave two inflection points.

The sixth lens element 560 has negative refractive power and it is madeof plastic material. The sixth lens element 560 has a convex object-sidesurface 562 and a concave image-side surface 564. Hereby, the back focallength is reduced to miniaturize the lens element effectively. Inaddition, the object-side surface 562 has two inflection points and theimage-side surface 564 has an inflection point, such that the angle ofincident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 580 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 560 and the image plane 590.

In the optical image capturing system of the fifth embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=62.245 mm andf5/ΣPP=0.083. Hereby, it is favorable for allocating the positiverefractive power of the first lens element 510 to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the fifth embodiment, sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−19.759 mm andf6/ΣNP=0.321. Hereby, it is favorable for allocating the negativerefractive power of the sixth lens element 560 to other negative lenselements.

Please refer to the following Table 9 and Table 10.

The detailed data of the optical image capturing system of the fifthembodiment is as shown in Table 9.

TABLE 9 Data of the optical image capturing system f = 5.855 mm; f/HEP =1.394; HAF = 40.000 deg Focal Surface# Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano At infinity 1 Ape. StopPlano −0.230 2 Lens 1 5.688631741 1.171 Plastic 1.544 55.96 20.429 310.77040524 0.000 4 Shading Plano 0.352 sheet 5 Lens 2 7.741772515 1.439Plastic 1.544 55.96 10.480 6 −20.45895021 0.967 7 Lens 3 −2.3038656230.444 Plastic 1.642 22.47 −13.425 8 −3.372040441 0.030 9 Lens 4−4.188477782 1.044 Plastic 1.544 55.96 26.192 10 −3.52436797 0.025 11Lens 5 2.782332783 0.572 Plastic 1.626 25.13 5.145 12 17.92751098 0.03013 Lens 6 5.085960421 0.792 Plastic 1.642 22.46 −6.333 14 2.1316208771.082 15 IR-bandstop Plano 0.200 1.517 64.13 filter 16 Plano 1.419 17Image plane Plano 0.000 Reference wavelength (d-line) = 555 nm, shieldposition: clear aperture (CA) of the fourth plano = 2.300 mm; clearaperture (CA) of the twelve plano = 3.750 mmAs for the parameters of the aspheric surfaces of the fifth embodiment,reference is made to Table 10.

TABLE 10 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k −1.875231E+007.602000E−11 4.562725E−07 −3.853899E+01 −4.388169E−01 −4.322673E+00−3.098350E+01 A4 −2.310956E−03 −1.334914E−02 −1.286689E−02 −7.856385E−03−4.951952E−02 −4.263075E−02 2.388939E−02 A6 −6.955452E−04 −7.408855E−04−1.937201E−04 −3.575284E−03 1.905849E−02 1.467458E−02 −5.225598E−03 A81.347015E−04 −8.641666E−05 −8.366123E−04 8.416503E−04 −1.231920E−04−1.986984E−03 −8.914323E−05 A10 −5.037430E−05 3.334804E−05 2.621781E−04−1.790009E−04 −9.544647E−04 1.119081E−04 2.096266E−04 A12 4.946612E−06−4.530866E−06 −4.669006E−05 2.876966E−05 2.040919E−04 −2.720705E−06−4.749368E−05 A14 −1.102954E−07 2.794439E−07 4.577708E−06 −2.524377E−06−1.794001E−05 9.331968E−08 4.761921E−06 A16 −5.231827E−08 −5.570000E−12−1.647328E−07 8.839127E−08 6.105240E−07 −5.376200E−10 −1.735218E−07Surface # 10 11 12 13 14 k −3.519849E−01 −9.662687E+00 4.941888E+000.000000E+00 −3.319878E+00 A4 3.280521E−03 1.417206E−03 3.859572E−023.358710E−02 4.262080E−03 A6 6.093040E−03 −1.101646E−03 −1.605214E−02−1.663012E−02 −3.427602E−03 A8 −2.773910E−03 8.759864E−05 3.420292E−033.403089E−03 6.444417E−04 A10 6.154473E−04 −5.215772E−06 −4.288114E−04−3.980020E−04 −6.582736E−05 A12 −8.202399E−05 1.179301E−06 3.174507E−052.717141E−05 3.802360E−06 A14 6.126318E−06 −1.426948E−07 −1.302425E−06−1.011725E−06 −1.157706E−07 A16 −1.867446E−07 5.144910E−09 2.283847E−081.584279E−08 1.433440E−09

The presentation of the aspheric surface formula in the fifth embodimentis similar to that in the first embodiment. Besides the definitions ofparameters in following tables are equal to those in the firstembodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 9 and Table 10.

Fifth embodiment (Primary reference wavelength: 587.5 nm) ETP1 ETP2 ETP3ETP4 ETP5 ETP6 0.789 1.117 0.838 0.666 0.421 1.004 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 0.674 0.776 1.886 0.638 0.736 1.268ETL EBL EIN EIR PIR EIN/ETL 9.303 2.016 7.287 0.397 1.082 0.783 SETP/EINEIR/PIR SETP STP SETP/STP BL 0.663 0.367 4.834 5.462 0.885 2.702 ED12ED23 ED34 ED45 ED56 EBL/BL 0.396 0.297 0.547 0.983 0.231 0.7461 SED SINSED/SIN 2.453 1.404 1.747 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45ED56/IN56 1.124 0.307 18.236 39.305 7.748 |f/f1| |f/f2| |f/f3| |f/f4||f/f5| |f/f6| 0.28660 0.55869 0.43611 0.22353 1.13791 0.92443TP4/(IN34 + Σ PPR Σ NPR Σ PPR/|Σ NPR| IN12/f IN56/f TP4 + IN45) 2.142761.42451 1.50421 0.06012 0.00508 0.94995 |f1/f2| |f2/f3| (TP1 + IN12)/TP2(TP6 + IN56)/TP5 1.94936 0.78059 1.05858 1.43723 HOS InTL HOS/HOIInS/HOS ODT % TDT % 9.56746 6.86592 1.91349 0.97597 2.34742 0.57085HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 2.79348 3.05681 3.255803.59517 0.71903 0.37577 |InRS62|/ TP2/TP3 TP3/TP4 InRS61 InRS62|InRS61|/TP6 TP6 3.23816 0.42571 0.49475 0.81085 0.62482 1.02402 MTFE0MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.57 0.43 0.29 0.24 0.09 0.15 MTFI0 MTFI3MTFI7 0.4 0.24 0.24

The following contents may be deduced from Table 9 and Table 10.

Related inflection point values of fifth embodiment (Primary referencewavelength: 555 nm) HIF111 1.4868 HIF111/HOI 0.2974 SGI111 0.1737|SGI111|/(|SGI111| + TP1) 0.1292 HIF121 0.7348 HIF121/HOI 0.1470 SGI1210.0211 |SGI121|/(|SGI121| + TP1) 0.0177 HIF211 0.8631 HIF211/HOI 0.1726SGI211 0.0408 |SGI211|/(|SGI211| + TP2) 0.0276 HIF311 2.1654 HIF311/HOI0.4331 SGI311 −1.1193 |SGI311|/(|SGI311| + TP3) 0.7158 HIF321 1.6360HIF321/HOI 0.3272 SGI321 −0.4515 |SGI321|/(|SGI321| + TP3) 0.5040 HIF3222.1113 HIF322/HOI 0.4223 SGI322 −0.6781 |SGI322|/(|SGI322| + TP3) 0.6041HIF411 0.68091 HIF411/HOI 0.13618 SGI411 −0.04271 |SGI411|/(|SGI411| +TP4) 0.03931 HIF412 1.48844 HIF412/HOI 0.29769 SGI412 −0.10092|SGI412|/(|SGI412| + TP4) 0.08816 HIF413 2.60726 HIF413/HOI 0.52145SGI413 −0.32505 |SGI413|/(|SGI413| + TP4) 0.23746 HIF421 2.50773HIF421/HOI 0.50155 SGI421 −0.76788 |SGI421|/(|SGI421| + TP4) 0.42385HIF511 1.40945 HIF511/HOI 0.28189 SGI511 0.25364 |SGI511|/(|SGI511| +TP5) 0.30734 HIF512 3.50009 HIF512/HOI 0.70002 SGI512 0.31907|SGI512|/(|SGI512| + TP5) 0.35821 HIF521 1.95980 HIF521/HOI 0.39196SGI521 0.24179 |SGI521|/(|SGI521| + TP5) 0.29724 HIF522 3.67720HIF522/HOI 0.73544 SGI522 0.19287 |SGI522|/(|SGI522| + TP5) 0.25227HIF611 1.59124 HIF611/HOI 0.31825 SGI611 0.30568 |SGI611|/(|SGI611| +TP6) 0.27852 HIF612 3.86544 HIF612/HOI 0.77309 SGI612 0.51337|SGI612|/(|SGI612| + TP6) 0.39332 HIF621 1.57642 HIF621/HOI 0.31528SGI621 0.45806 |SGI621|/(|SGI621| + TP6) 0.36648

The Sixth Embodiment Embodiment 6

Please refer to FIG. 6A, FIG. 6B, FIGS. 6C, and 6D. FIG. 6A is aschematic view of the optical image capturing system according to thesixth Embodiment of the present application, FIG. 6B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the sixth Embodiment of the presentapplication, FIG. 6C is a characteristic diagram of modulation transferof a visible light according to the sixth embodiment of the presentapplication and FIG. 6D is a characteristic diagram of modulationtransfer of infrared rays according to the sixth embodiment of thepresent application. As shown in FIG. 6A, in order from an object sideto an image side, the optical image capturing system includes anaperture stop 600, a first lens element 610, a second lens element 620,a third lens element 630, a fourth lens element 640, a fifth lenselement 650, a sixth lens element 660, an IR-bandstop filter 680, animage plane 690, and an image sensing device 692.

The first lens element 610 has positive refractive power and it is madeof plastic material. The first lens element 610 has a convex object-sidesurface 612 and a concave image-side surface 614, and both of theobject-side surface 612 and the image-side surface 614 are aspheric andhave an inflection point.

The second lens element 620 has positive refractive power and it is madeof plastic material. The second lens element 620 has a convexobject-side surface 622 and a convex image-side surface 624, and both ofthe object-side surface 622 and the image-side surface 624 are aspheric.The object-side surface 622 has an inflection point.

The third lens element 630 has negative refractive power and it is madeof plastic material. The third lens element 630 has a concaveobject-side surface 632 and a convex image-side surface 634, and both ofthe object-side surface 632 and the image-side surface 634 are asphericand have an inflection point.

The fourth lens element 640 has positive refractive power and it is madeof plastic material. The fourth lens element 640 has a concaveobject-side surface 642 and a convex image-side surface 644, and both ofthe object-side surface 642 and the image-side surface 644 are aspheric.The object-side surface 642 has three inflection points and theimage-side surface 644 has an inflection point.

The fifth lens element 650 has positive refractive power and it is madeof plastic material. The fifth lens element 650 has a convex object-sidesurface 652 and a concave image-side surface 654, and both of theobject-side surface 652 and the image-side surface 654 are aspheric. Theobject-side surface 652 has three inflection points and the image-sidesurface 654 both have four inflection points.

The sixth lens element 660 has negative refractive power and it is madeof plastic material. The sixth lens element 660 has a convex object-sidesurface 662 and a concave image-side surface 664. The object-sidesurface 662 has three inflection points and the image-side surface 664has an inflection point. Hereby, the back focal length is reduced tominiaturize the lens element effectively. In addition, the angle ofincident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 680 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 660 and the image plane 690.

In the optical image capturing system of the sixth Embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=136.278 mm andf1/ΣPP=0.59. Hereby, it is favorable for allocating the positiverefractive power of the first lens element 610 to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the sixth Embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=−15.260 mm andf6/ΣNP=0.492. Hereby, it is favorable for allocating the negativerefractive power of the sixth lens element 660 to other negative lenselements.

Please refer to the following Table 11 and Table 12.

The detailed data of the optical image capturing system of the sixthEmbodiment is as shown in Table 11.

TABLE 11 Data of the optical image capturing system f = 5.865 mm; f/HEP= 1.6; HAF = 40.000 deg Focal Surface# Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano At infinity 1 Ape. StopPlano −0.010 2 Lens 1 7.415294123 0.980 Plastic 1.522 56.40 113.017 38.09319088 0.000 4 Shading Plano 0.221 sheet 5 Lens 2 5.66634217 1.563Plastic 1.544 55.96 7.106 6 −11.09480586 0.927 7 Lens 3 −1.7176302620.500 Plastic 1.642 22.47 −7.745 8 −2.910968551 0.030 9 Lens 4−17.86380269 1.451 Plastic 1.544 55.96 8.123 10 −3.653819316 0.025 11Lens 5 3.324994761 0.629 Plastic 1.642 22.47 8.031 12 8.531738704 0.03013 Lens 6 4.158484856 0.735 Plastic 1.642 22.47 −7.515 14 2.0866299341.288 15 IR-bandstop Plano 0.200 1.517 64.13 filter 16 Plano 1.420 17Image plane Plano Reference wavelength (d-line) = 555 nm, shieldposition: clear aperture (CA) of the fourth plano = 2.175 mm; clearaperture (CA) of the twelve plano = 3.850 mmAs for the parameters of the aspheric surfaces of the sixth Embodiment,reference is made to Table 12.

TABLE 12 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k −1.564355E+007.602000E−11 4.690128E−07 −3.853899E+01 −6.447823E−01 −6.206438E−01−5.310210E+00 A4 −7.038659E−03 −3.412654E−02 −2.826543E−02 −1.463575E−026.124900E−03 9.433790E−03 2.705841E−02 A6 −3.121781E−05 2.565804E−03−6.368931E−04 −1.678404E−03 4.883579E−03 −2.587088E−03 −1.132676E−02 A8−8.807667E−05 −1.536710E−03 2.199370E−04 −6.447841E−04 −1.552079E−032.050712E−03 3.095691E−03 A10 −5.969774E−05 6.517718E−04 −5.260127E−043.425155E−04 5.244909E−04 −6.810266E−04 −5.540890E−04 A12 3.017221E−06−1.318713E−04 3.054776E−04 −4.597253E−05 −1.130668E−04 1.069880E−045.536016E−05 A14 4.301450E−06 1.191670E−05 −6.551663E−05 5.867509E−071.293203E−05 −8.193522E−06 −2.723375E−06 A16 −1.030206E−06 −4.962808E−074.666260E−06 1.720163E−07 −5.408195E−07 2.522622E−07 5.112022E−08Surface # 10 11 12 13 14 k −7.207911E−01 −1.912912E+00 3.407383E+000.000000E+00 −1.092240E+00 A4 1.673737E−02 −4.474499E−03 2.517171E−021.839988E−02 −1.955608E−02 A6 −7.368828E−03 −4.768722E−03 −1.101951E−02−8.188872E−03 2.490384E−03 A8 2.294498E−03 1.594205E−03 2.333761E−031.526968E−03 −3.973040E−04 A10 −3.946628E−04 −2.543423E−04 −3.113201E−04−1.932188E−04 3.998842E−05 A12 3.750065E−05 2.261875E−05 2.464584E−051.422273E−05 −2.270287E−06 A14 −1.849829E−06 −1.053786E−06 −1.028293E−06−5.269318E−07 6.849812E−08 A16 3.818065E−08 1.982533E−08 1.721031E−087.443330E−09 −8.617500E−10

In the sixth Embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 11 and Table 12.

Sixth embodiment (Primary reference wavelength: 555 nm) ETP1 ETP2 ETP3ETP4 ETP5 ETP6 0.730 1.250 0.928 1.054 0.533 0.911 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 0.745 0.800 1.855 0.726 0.848 1.239ETL EBL EIN EIR PIR EIN/ETL 9.884 2.280 7.604 0.660 1.288 0.769 SETP/EINEIR/PIR SETP STP SETP/STP BL 0.711 0.512 5.406 5.858 0.923 2.908 ED12ED23 ED34 ED45 ED56 EBL/BL 0.319 0.345 0.541 0.780 0.214 0.7840 SED SINSED/SIN 1.199 1.234 1.782 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45ED56/IN56 1.440 0.372 18.047 31.181 7.127 |f/f1| |f/f2| |f/f3| |f/f4||f/f5| |f/f6| 0.05189 0.82532 0.75724 0.72200 0.73026 0.78046TP4/(IN34 + Σ PPR Σ NPR Σ PPR/|Σ NPR| IN12/f IN56/f TP4 + IN45) 2.329461.53770 1.51490 0.03775 0.00511 0.96349 |f1/f2| |f2/f3| (TP1 + IN12)/TP2(TP6 + IN56)/TP5 15.90380 0.91752 0.76875 1.21625 HOS InTL HOS/HOIInS/HOS ODT % TDT % 10.00000 7.09171 2.00000 0.99900 1.62151 0.66113HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 2.79348 3.05681 3.255803.59517 0.71903 0.37577 |InRS62|/ TP2/TP3 TP3/TP4 InRS61 InRS62|InRS61|/TP6 TP6 3.23816 0.42571 0.49475 0.81085 0.62482 1.02402 MTFE0MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.81 0.67 0.5 0.53 0.25 0.23 MTFI0 MTFI3MTFI7 0.38 0.42 0.31

The following contents may be deduced from Table 11 and Table 12.

Related inflection point values of sixth Embodiment (Primary referencewavelength: 555 nm) HIF111 1.1352 HIF111/HOI 0.2270 SGI111 0.0744|SGI111|/(|SGI111| + TP1) 0.0706 HIF121 0.5634 HIF121/HOI 0.1127 SGI1210.0163 |SGI121|/(|SGI121| + TP1) 0.0163 HIF211 0.7189 HIF211/HOI 0.1438SGI211 0.0382 |SGI211|/(|SGI211| + TP2) 0.0238 HIF311 2.11642 HIF311/HOI0.42328 SGI311 −1.20372 |SGI311|/(|SGI311| + TP3) 0.70652 HIF321 2.51154HIF321/HOI 0.50231 SGI321 −0.88542 |SGI321|/(|SGI321| + TP3) 0.63910HIF411 0.46382 HIF411/HOI 0.09276 SGI411 −0.00487 |SGI411|/(|SGI411| +TP4) 0.00334 HIF412 1.56361 HIF412/HOI 0.31272 SGI412 0.00101|SGI412|/(|SGI412| + TP4) 0.00069 HIF413 2.67820 HIF413/HOI 0.53564SGI413 −0.07265 |SGI413|/(|SGI413| + TP4) 0.04767 HIF421 2.48609HIF421/HOI 0.49722 SGI421 −0.65230 |SGI421|/(|SGI421| + TP4) 0.31008HIF511 1.38653 HIF511/HOI 0.27731 SGI511 0.24417 |SGI511|/(|SGI511| +TP5) 0.27965 HIF512 2.73953 HIF512/HOI 0.54791 SGI512 0.55524|SGI512|/(|SGI512| + TP5) 0.46888 HIF513 3.16694 HIF513/HOI 0.63339SGI513 0.63515 |SGI513|/(|SGI513| + TP5) 0.50245 HIF521 1.76665HIF521/HOI 0.35333 SGI521 0.25187 |SGI521|/(|SGI521| + TP5) 0.28595HIF522 2.88834 HIF522/HOI 0.57767 SGI522 0.47213 |SGI522|/(|SGI522| +TP5) 0.42879 HIF523 3.57692 HIF523/HOI 0.71538 SGI523 0.61663|SGI523|/(|SGI523| + TP5) 0.49505 HIF524 3.80969 HIF524/HOI 0.76194SGI524 0.68822 |SGI524|/(|SGI524| + TP5) 0.52250 HIF611 1.83748HIF611/HOI 0.36750 SGI611 0.45477 |SGI611|/(|SGI611| + TP6) 0.38223HIF612 3.22181 HIF612/HOI 0.64436 SGI612 0.74837 |SGI612|/(|SGI612| +TP6) 0.50451 HIF613 3.81117 HIF613/HOI 0.76223 SGI613 0.76402|SGI613|/(|SGI613| + TP6) 0.50968 HIF621 1.81033 HIF621/HOI 0.36207SGI621 0.61649 |SGI621|/(|SGI621| + TP6) 0.45615

The Seventh Embodiment Embodiment 7

Please refer to FIG. 7A and FIG. 7B, FIGS. 7C, and 7D. FIG. 7A is aschematic view of the optical image capturing system according to theseventh Embodiment of the present application, FIG. 7B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the seventh Embodiment of the presentapplication, FIG. 7C is a characteristic diagram of modulation transferof a visible light according to the seventh embodiment of the presentapplication and FIG. 7D is a characteristic diagram of modulationtransfer of infrared rays according to the seventh embodiment of thepresent application. As shown in FIG. 7A, in order from an object sideto an image side, the optical image capturing system includes anaperture stop 700, a first lens element 710, a second lens element 720,a third lens element 730, a fourth lens element 740, a fifth lenselement 750, a sixth lens element 760, an IR-bandstop filter 780, animage plane 790, and an image sensing device 792.

The first lens element 710 has positive refractive power and it is madeof plastic material. The first lens element 710 has a convex object-sidesurface 712 and a concave image-side surface 714, and both of theobject-side surface 712 and the image-side surface 714 are aspheric. Theimage-side surface 714 has an inflection point.

The second lens element 720 has negative refractive power and it is madeof plastic material. The second lens element 720 has a concaveobject-side surface 722 and a convex image-side surface 724, and both ofthe object-side surface 722 and the image-side surface 724 are aspheric.The image-side surface 724 has an inflection point.

The third lens element 730 has positive refractive power and it is madeof plastic material. The third lens element 730 has a convex object-sidesurface 732 and a concave image-side surface 734, and both of theobject-side surface 732 and the image-side surface 734 are aspheric andhave an inflection point.

The fourth lens element 740 has negative refractive power and it is madeof plastic material. The fourth lens element 740 has a concaveobject-side surface 742 and a concave image-side surface 744, and bothof the object-side surface 742 and the image-side surface 744 areaspheric. The image-side surface 744 has an inflection point.

The fifth lens element 750 has positive refractive power and it is madeof plastic material. The fifth lens element 750 has a convex object-sidesurface 752 and a convex image-side surface 754, and both of theobject-side surface 752 and the image-side surface 754 are aspheric andhave an inflection point.

The sixth lens element 760 has negative refractive power and it is madeof plastic material. The sixth lens element 760 has a concaveobject-side surface 762 and a concave image-side surface 764. Theobject-side surface 762 and the image-side surface 764 both have aninflection point. Hereby, the back focal length is reduced tominiaturize the lens element effectively. In addition, the angle ofincident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 780 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 760 and the image plane 790.

In the optical image capturing system of the seventh Embodiment, a sumof focal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=33.021 mm andf5/ΣPP=0.67. Hereby, it is favorable for allocating the positiverefractive power of the first lens element 710 to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the seventh Embodiment, a sumof focal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=−76.566 mm andf6/ΣNP=0.038. Hereby, it is favorable for allocating the negativerefractive power of the sixth lens element 760 to other negative lenselements.

Please refer to the following Table 13 and Table 14.

The detailed data of the optical image capturing system of the seventhEmbodiment is as shown in Table 13.

TABLE 13 Data of the optical image capturing system f = 4.090 mm; f/HEP= 1.4; HAF = 50.000 deg Focal Surface# Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano At infinity 1 Ape. StopPlano −0.41968 2 Lens 1 2.90789 0.520564 Plastic 1.565 58 8.02124 37.54644 0.684636 4 Lens 2 −4.002 0.165 Plastic 1.632 23.4 −61.8084 5−4.52639 0.050029 6 Lens 3 12.29981 0.562066 Plastic 1.565 58 22.785 7254.319 0.211468 8 Lens 4 −13.4774 0.402178 Plastic 1.607 26.6 −11.87869 15.91132 0.208877 10 Lens 5 5.91704 1.204943 Plastic 1.607 26.62.21514 11 −1.61968 0.395715 12 Lens 6 −2.92658 0.52911 Plastic 1.60726.6 −2.87888 13 4.71344 0.5 14 IR-bandstop Plano 0.2 1.517 64.13 filter15 Plano 0.846796 16 Image plane Plano Reference wavelength = 555 nmAs for the parameters of the aspheric surfaces of the seventhEmbodiment, reference is made to Table 14.

TABLE 14 Aspheric Coefficients Surface # 2 3 4 5 6 7 8 k −8.575082−48.928008 3.035604 −1.87003 9.002997 50.000222 43.827767 A4 4.09973E−022.02034E−02 4.35142E−03 −5.29328E−03 −2.38607E−02 −4.75064E−03−1.01342E−02 A6 −2.44804E−03 −6.02206E−03 7.26270E−03 4.60735E−039.95969E−04 −7.70915E−03 −1.69683E−03 A8 −2.97169E−03 −2.08058E−04−4.13563E−03 3.03213E−03 −1.44437E−03 −4.49698E−04 −1.70152E−04 A109.99941E−04 7.08432E−04 1.19653E−03 −3.82747E−04 1.31541E−04−7.96902E−05 −1.08190E−04 A12 4.26638E−04 2.32538E−04 4.96634E−04−2.00672E−04 4.83672E−05 −1.06955E−05 −3.91368E−05 A14 −1.84430E−04−2.26808E−04 −3.33707E−04 3.07381E−05 −4.47241E−05 −3.81151E−061.90658E−05 Surface # 9 10 11 12 13 k 27.972506 −50 −3.11971 −7.448356−8.337328 A4 −4.42341E−02 −2.20803E−02 −9.40106E−03 1.22566E−02−4.44170E−03 A6 2.09966E−03 1.74461E−04 4.22751E−04 −5.09253E−03−4.87237E−04 A8 −5.80191E−05 1.71535E−04 6.02212E−05 1.43676E−042.35278E−05 A10 1.06706E−05 9.09135E−07 2.34225E−06 2.63513E−054.31019E−07 A12 −5.97760E−07 −6.21206E−06 3.08205E−07 1.51313E−069.62397E−09 A14 −5.34708E−06 −1.90980E−06 1.93745E−07 −2.14347E−07−3.53037E−09

In the seventh Embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 13 and Table 14.

Seventh embodiment (Primary reference wavelength: 555 nm) ETP1 ETP2 ETP3ETP4 ETP5 ETP6 0.243 0.268 0.493 0.456 0.647 0.969 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 0.468 1.626 0.876 1.133 0.537 1.832ETL EBL EIN EIR PIR EIN/ETL 6.062 1.375 4.687 0.328 0.500 0.773 SETP/EINEIR/PIR SETP STP SETP/STP BL 0.656 0.656 3.076 3.384 0.909 1.547 ED12ED23 ED34 ED45 ED56 EBL/BL 0.262 0.189 0.154 0.344 0.662 0.8888 SED SINSED/SIN 1.611 1.551 1.039 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45ED56/IN56 0.383 3.784 0.727 1.647 1.672 |f/f1| |f/f2| |f/f3| |f/f4||f/f5| |f/f6| 0.50986 0.06617 0.17949 0.34429 1.84624 1.42058TP4/(IN34 + Σ PPR Σ NPR Σ PPR/|Σ NPR| IN12/f IN56/f TP4 + IN45) 4.120980.37543 10.97658 0.16741 0.09676 0.48896 |f1/f2| |f2/f3| (TP1 +IN12)/TP2 (TP6 + IN56)/TP5 0.12978 2.71268 7.30424 0.76753 HOS InTLHOS/HOI InS/HOS ODT % TDT % 6.48138 4.93459 1.29628 0.93525 2.05011.01082 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 1.09927 0 0.000002.20291 0.44058 0.33988 |InRS61|/ |InRS62|/ TP2/TP3 TP3/TP4 InRS61InRS62 TP6 TP6 0.29356 1.39756 −1.28432 −0.86678 2.42732 1.63818 MTFE0MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.33 0.05 0.05 0.25 0.07 0.13 MTFI0 MTFI3MTFI7 0.45 0.03 0.22

The following contents may be deduced from Table 13 and Table 14.

Related inflection point values of seventh Embodiment (Primary referencewavelength: 555 nm) HIF121 1.24814 HIF121/HOI 0.24963 SGI121 0.11172|SGI121|/(|SGI121| + TP1) 0.17670 HIF221 1.01791 HIF221/HOI 0.20358SGI221 −0.11095 |SGI221|/(|SGI221| + TP2) 0.40207 HIF311 0.54279HIF311/HOI 0.10856 SGI311 0.00998 |SGI311|/(|SGI311| + TP3) 0.01744HIF321 0.23693 HIF321/HOI 0.04739 SGI321 0.00009 |SGI321|/(|SGI321| +TP3) 0.00017 HIF421 0.35030 HIF421/HOI 0.07006 SGI421 0.00321|SGI421|/(|SGI421| + TP4) 0.00791 HIF511 0.59426 HIF511/HOI 0.11885SGI511 0.0241121 |SGI511|/(|SGI511| + TP5) 0.01962 HIF521 1.91811HIF521/HOI 0.38362 SGI521 −0.84996 |SGI521|/(|SGI521| + TP5) 0.41363HIF611 2.47689 HIF611/HOI 0.49538 SGI611 −0.89345 |SGI611|/(|SGI611| +TP6) 0.62806 HIF621 1.24993 HIF621/HOI 0.24999 SGI621 0.135998|SGI621|/(|SGI621| + TP6) 0.20448

The Eight Embodiment Embodiment 8

Please refer to FIG. 8A, FIG. 8B, FIGS. 8C, and 8D. FIG. 8A is aschematic view of the optical image capturing system according to theeighth Embodiment of the present application, FIG. 8B is longitudinalspherical aberration curves, astigmatic field curves, and an opticaldistortion curve of the optical image capturing system in the order fromleft to right according to the eighth Embodiment of the presentapplication, FIG. 8C is a characteristic diagram of modulation transferof a visible light according to the eighth embodiment of the presentapplication and FIG. 8D is a characteristic diagram of modulationtransfer of infrared rays according to the eighth embodiment of thepresent application. As shown in FIG. 8A, in order from an object sideto an image side, the optical image capturing system includes anaperture stop 800, a first lens element 810, a second lens element 820,a third lens element 830, a fourth lens element 840, a fifth lenselement 850, a sixth lens element 860, an IR-bandstop filter 880, animage plane 890, and an image sensing device 892.

The first lens element 810 has positive refractive power and it is madeof plastic material. The first lens element 810 has a convex object-sidesurface 812 and a concave image-side surface 814, both of theobject-side surface 812 and the image-side surface 814 are aspheric, andthe image-side surface 814 has an inflection point.

The second lens element 820 has negative refractive power and it is madeof plastic material. The second lens element 820 has a concaveobject-side surface 822 and a concave image-side surface 824, and bothof the object-side surface 822 and the image-side surface 824 areaspheric. The image-side surface 824 has two inflection points.

The third lens element 830 has negative refractive power and it is madeof plastic material. The third lens element 830 has a convex object-sidesurface 832 and a concave image-side surface 834, and both of theobject-side surface 832 and the image-side surface 834 are aspheric. Theobject-side surface 832 and the image-side surface 834 both have aninflection point.

The fourth lens element 840 has positive refractive power and it is madeof plastic material. The fourth lens element 840 has a concaveobject-side surface 842 and a convex image-side surface 844, and both ofthe object-side surface 842 and the image-side surface 844 are aspheric.The object-side surface 842 has three inflection points.

The fifth lens element 850 has positive refractive power and it is madeof plastic material. The fifth lens element 850 has a convex object-sidesurface 852 and a convex image-side surface 854, and both of theobject-side surface 852 and the image-side surface 854 are aspheric. Theobject-side surface 852 has three inflection pints and the image-sidesurface 854 has an inflection point.

The sixth lens element 860 has negative refractive power and it is madeof plastic material. The sixth lens element 860 has a concaveobject-side surface 862 and a concave image-side surface 864. Theobject-side surface 862 has two inflection points and the image-sidesurface 864 has an inflection point. Hereby, the back focal length isreduced to miniaturize the lens element effectively. In addition, theangle of incident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 880 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 860 and the image plane 890.

In the optical image capturing system of the eighth Embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=12.785 mm andf5/ΣPP=0.10. Hereby, it is favorable for allocating the positiverefractive power of the first lens element 810 to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the eighth Embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=−112.117 mm andf6/ΣNP=0.009. Hereby, it is favorable for allocating the negativerefractive power of the sixth lens element 860 to other negative lenselements.

Please refer to the following Table 15 and Table 16.

The detailed data of the optical image capturing system of the eighthEmbodiment is as shown in Table 15.

TABLE 15 Data of the optical image capturing system f = 3.213 mm; f/HEP= 2.4; HAF = 50.015 deg Focal Surface# Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano At infinity 1 Shading Plano0.000 sheet 2 Ape. Stop Plano −0.108 3 Lens 1 2.117380565 0.267 Plastic1.565 58.00 6.003 4 5.351202213 0.632 5 Lens 2 −70.37596785 0.230Plastic 1.517 21.40 −11.326 6 8.30936549 0.050 7 Lens 3 7.3331718650.705 Plastic 1.565 58.00 −99.749 8 6.265499794 0.180 9 Lens 4−71.32533363 0.832 Plastic 1.565 58.00 5.508 10 −3.003657909 0.050 11Lens 5 3.397431079 0.688 Plastic 1.583 30.20 1.274 12 −0.886432266 0.05013 Lens 6 −3.715425702 0.342 Plastic 1.650 21.40 −1.042 14 0.8676236370.700 15 IR-bandstop Plano 0.200 1.517 64.13 filter 16 Plano 0.407 17Image plane Plano Reference wavelength = 555 nm; shield position: clearaperture (CA) of the first plano = 0.640 mmAs for the parameters of the aspheric surfaces of the eighth Embodiment,reference is made to Table 16.

TABLE 16 Aspheric Coefficients Surface# 3 4 5 6 7 8 9 k −1.486403E+002.003790E+01 −4.783682E+01 −2.902431E+01 −5.000000E+01 −5.000000E+01−5.000000E+01 A4 2.043654E−02 −2.642626E−02 −6.237485E−02 −4.896336E−02−7.363667E−02 −5.443257E−02 3.105497E−02 A6 −2.231403E−04 −4.147746E−02−8.137705E−02 −1.981368E−02 1.494245E−02 1.263891E−04 −1.532514E−02 A8−1.387235E−02 2.901026E−02 4.589961E−02 3.312952E−03 6.252296E−03−9.655324E−03 −6.443603E−04 A10 −3.431740E−02 −9.512960E−02−5.485574E−02 5.634445E−03 −2.226544E−03 1.318692E−03 4.321089E−04 A120.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface # 10 11 1213 14 k 8.520005E−01 −5.000000E+01 −4.524978E+00 −5.000000E+01−4.286435E+00 A4 −6.786287E−03 −9.520247E−02 −4.666187E−02 5.856863E−03−2.635938E−02 A6 6.693976E−03 −5.507560E−05 3.849227E−03 2.442214E−033.694093E−03 A8 8.220809E−04 1.932773E−03 1.041053E−03 −2.201034E−03−1.355873E−04 A10 −2.798394E−04 3.346274E−04 4.713339E−06 −1.065215E−04−5.321575E−05 A12 0.000000E+00 1.125736E−05 −2.834871E−06 1.227641E−046.838440E−06 A14 0.000000E+00 −1.671951E−05 −2.293810E−06 −1.181115E−05−2.530792E−07

In the eighth Embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 15 and Table 16.

Eighth embodiment (Primary reference wavelength: 555 nm) ETP1 ETP2 ETP3ETP4 ETP5 ETP6 0.203 0.263 0.710 0.760 0.479 0.556 ETP1/TP1 ETP2/TP2ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 0.759 1.142 1.008 0.914 0.696 1.628ETL EBL EIN EIR PIR EIN/ETL 5.234 1.134 4.100 0.527 0.700 0.783 SETP/EINEIR/PIR SETP STP SETP/STP BL 0.725 0.753 2.971 3.064 0.970 1.304 ED12ED23 ED34 ED45 ED56 EBL/BL 0.580 0.050 0.161 0.150 0.188 0.8696 SED SINSED/SIN 1.129 0.962 1.173 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45ED56/IN56 0.917 1.005 0.896 2.997 3.756 |f/f1| |f/f2| |f/f3| |f/f4||f/f5| |f/f6| 0.53529 0.28371 0.03221 0.58335 2.52139 3.08263TP4/(IN34 + Σ PPR Σ NPR Σ PPR/|Σ NPR| IN12/f IN56/f TP4 + IN45) 6.722660.84594 7.94700 0.19680 0.01556 0.78362 |f1/f2| |f2/f3| (TP1 + IN12)/TP2(TP6 + IN56)/TP5 0.53001 0.11354 3.90947 0.56888 HOS InTL HOS/HOIInS/HOS ODT % TDT % 5.33002 4.02576 1.36178 0.97981 1.92371 1.09084HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 0.67483 0 0.00000 2.239650.57222 0.42020 |InRS61|/ |InRS62|/ TP2/TP3 TP3/TP4 InRS61 InRS62 TP6TP6 0.32631 0.84713 −0.74088 −0.06065 2.16896 0.17755 MTFE0 MTFE3 MTFE7MTFQ0 MTFQ3 MTFQ7 0.9 0.85 0.8 0.77 0.63 0.51 MTFI0 MTFI3 MTFI7 0.450.03 0.22

The following contents may be deduced from Table 15 and Table 16.

Related inflection point values of eighth Embodiment (Primary referencewavelength: 555 nm) HIF121 0.57452 HIF121/HOI 0.14679 SGI121 0.02858|SGI121|/(|SGI121| + TP1) 0.09675 HIF221 0.40206 HIF221/HOI 0.10272SGI221 0.00821 |SGI221|/(|SGI221| + TP2) 0.03448 HIF222 1.11769HIF222/HOI 0.28556 SGI222 −0.02234 |SGI222|/(|SGI222| + TP2) 0.08853HIF311 0.37391 HIF311/HOI 0.09553 SGI311 0.00785 |SGI311|/(|SGI311| +TP3) 0.01102 HIF321 0.42061 HIF321/HOI 0.10746 SGI321 0.01170|SGI321|/(|SGI321| + TP3) 0.01633 HIF411 0.19878 HIF411/HOI 0.05079SGI411 −0.00023 |SGI411|/(|SGI411| + TP4) 0.00028 HIF412 0.87349HIF412/HOI 0.22317 SGI412 0.00583 |SGI412|/(|SGI412| + TP4) 0.00695HIF413 1.87638 HIF413/HOI 0.47940 SGI413 −0.17360 |SGI413|/(|SGI413| +TP4) 0.17263 HIF511 0.36373 HIF511/HOI 0.09293 SGI511 0.015644|SGI511|/(|SGI511| + TP5) 0.02222 HIF512 1.7159 HIF512/HOI 0.43840SGI512 −0.446747 |SGI512|/(|SGI512| + TP5) 0.39358 HIF513 1.93653HIF513/HOI 0.49477 SGI513 −0.638544 |SGI513|/(|SGI513| + TP5) 0.48124HIF521 1.54767 HIF521/HOI 0.39542 SGI521 −0.792114 |SGI521|/(|SGI521| +TP5) 0.53505 HIF611 0.82168 HIF611/HOI 0.20993 SGI611 −0.060958|SGI611|/(|SGI611| + TP6) 0.15143 HIF612 0.98146 HIF612/HOI 0.25076SGI612 −0.07785 |SGI612|/(|SGI612| + TP6) 0.18561 HIF621 0.79476HIF621/HOI 0.20306 SGI621 0.238143 |SGI621|/(|SGI621| + TP6) 0.41079

The above-mentioned descriptions represent merely the exemplaryembodiment of the present disclosure, without any intention to limit thescope of the present disclosure thereto. Various equivalent changes,alternations or modifications based on the claims of present disclosureare all consequently viewed as being embraced by the scope of thepresent disclosure.

What is claimed is:
 1. An optical image capturing system, from an objectside to an image side, comprising: a first lens element with refractivepower; a second lens element with refractive power; a third lens elementwith refractive power; a fourth lens element with refractive power; afifth lens element with refractive power; a sixth lens element withrefractive power; and an image plane; wherein the optical imagecapturing system consists of six lens elements with refractive power, amaximum height for image formation on the image plane perpendicular tothe optical axis in the optical image capturing system is denoted byHOI, at least two lens elements among the first through sixth lenselements respectively have at least one inflection point on at least onesurface thereof, at least one of the first through sixth lens elementshas positive refractive power, an object-side surface and an image-sidesurface of the sixth lens element are aspheric, focal lengths of thefirst through sixth lens elements are f1, f2, f3, f4, f5 and f6respectively, a focal length of the optical image capturing system is f,an entrance pupil diameter of the optical image capturing system is HEP,a distance on an optical axis from an axial point on an object-sidesurface of the first lens element to an axial point on the image planeis HOS, thicknesses in parallel with an optical axis of the firstthrough sixth lens elements at height ½ HEP respectively are ETP1, ETP2,ETP3, ETP4, ETP5 and ETP6, a sum of ETP1 to ETP6 described above isSETP, thicknesses of the first through sixth lens elements on theoptical axis respectively are TP1, TP2, TP3, TP4, TP5 and TP6, a sum ofTP1 to TP6 described above is STP, and the following relations aresatisfied: 1.2≦f/HEP≦6.0 and 0.5≦SETP/STP<1.
 2. The optical imagecapturing system of claim 1, wherein a horizontal distance in parallelwith the optical axis from a coordinate point on the object-side surfaceof the first lens element at height ½ HEP to the image plane is ETL, ahorizontal distance in parallel with the optical axis from a coordinatepoint on the object-side surface of the first lens element at height ½HEP to a coordinate point on the image-side surface of the sixth lenselement at height ½ HEP is EIN, and the following relation is satisfied:0.2≦EIN/ETL<1.
 3. The optical image capturing system of claim 2, whereinthe thicknesses in parallel with the optical axis of the first throughsixth lens elements at height ½ HEP respectively are ETP1, ETP2, ETP3,ETP4, ETP5 and ETP6, the sum of ETP1 to ETP6 described above is SETP,and the following relation is satisfied: 0.3≦SETP/EIN<1.
 4. The opticalimage capturing system of claim 1, wherein the optical image capturingsystem comprises a light filtration element, the light filtrationelement is located between the sixth lens element and the image plane, adistance in parallel with the optical axis from a coordinate point onthe image-side surface of the sixth lens element at height ½ HEP to thelight filtration element is EIR, a distance in parallel with the opticalaxis from an axial point on the image-side surface of the sixth lenselement to the light filtration element is PIR, and the followingrelation is satisfied: 0.1≦EIR/PIR≦1.1.
 5. The optical image capturingsystem of claim 1, wherein an object-side surface or an image-sidesurface of at least one of the six lens elements has at least twoinflection points.
 6. The optical image capturing system of claim 1,wherein contrast transfer rates of modulation transfer with spacefrequencies of 55 cycles/mm (MTF values) of a visible light at theoptical axis on the image plane, 0.3 HOI and 0.7 HOI are respectivelydenoted by MTFE0, MTFE3 and MTFE7, and the following relations aresatisfied: MTFE0≧0.2, MTFE3≧0.01 and MTFE7≧0.01.
 7. The optical imagecapturing system of claim 1, wherein a half of maximum view angle of theoptical image capturing system is HAF, and the following relation issatisfied: 0.4≦|tan(HAF)|≦6.0.
 8. The optical image capturing system ofclaim 1, wherein a horizontal distance in parallel with the optical axisfrom a coordinate point on the image-side surface of the sixth lenselement at height ½ HEP to the image plane is EBL, a horizontal distancein parallel with the optical axis from an axial point on the image-sidesurface of the sixth lens element to the image plane is BL, and thefollowing relation is satisfied: 0.2≦EBL/BL<1.1.
 9. The optical imagecapturing system of claim 1, further comprising an aperture stop, adistance from the aperture stop to the image plane on the optical axisis InS, an image sensing device is disposed on the image plane, and thefollowing relations are satisfied: 0.2≦InS/HOS≦1.1 and 0≦HIF/HOI≦0.9.10. An optical image capturing system, from an object side to an imageside, comprising: a first lens element with refractive power; a secondlens element with refractive power; a third lens element with refractivepower; a fourth lens element with refractive power; a fifth lens elementwith positive refractive power; a sixth lens element with negativerefractive power; and an image plane; wherein the optical imagecapturing system consists of six lens elements with refractive power, amaximum height for image formation on the image plane perpendicular tothe optical axis in the optical image capturing system is denoted byHOI, at least two lens elements among the six lens elements respectivelyhave at least one inflection point on at least one surface thereof, atleast one of the first through fourth lens elements has positiverefractive power, focal lengths of the first through sixth lens elementsare f1, f2, f3, f4, f5 and f6 respectively, a focal length of theoptical image capturing system is f, an entrance pupil diameter of theoptical image capturing system is HEP, a distance on an optical axisfrom an axial point on an object-side surface of the first lens elementto an axial point on the image plane is HOS, a horizontal distance inparallel with the optical axis from a coordinate point on theobject-side surface of the first lens element at height ½ HEP to theimage plane is ETL, a horizontal distance in parallel with the opticalaxis from a coordinate point on the object-side surface of the firstlens element at height ½ HEP to a coordinate point on the image-sidesurface of the sixth lens element at height ½ HEP is EIN, and thefollowing relations are satisfied: 1.2≦f/HEP≦6.0, HOI>3.0 mm and0.2≦EIN/ETL<1.
 11. The optical image capturing system of claim 10,wherein a horizontal distance in parallel with the optical axis from acoordinate point on the image-side surface of the fifth lens element atheight ½ HEP to a coordinate point on the object-side surface of thesixth lens element at height ½ HEP is ED56, a distance from the fifthlens element to the sixth lens element on the optical axis is IN56, andthe following relation is satisfied: 0<ED56/IN56≦50.
 12. The opticalimage capturing system of claim 10, wherein a horizontal distance inparallel with the optical axis from a coordinate point on the image-sidesurface of the first lens element at height ½ HEP to a coordinate pointon the object-side surface of the second lens element at height ½ HEP isED12, a distance from the first lens element to the second lens elementon the optical axis is IN12, and the following relation is satisfied:0<ED12/IN12<10.
 13. The optical image capturing system of claim 10,wherein a thickness in parallel with the optical axis of the second lenselement at height ½ HEP is ETP2, a thickness of the second lens elementon the optical axis is TP2, and the following relation is satisfied:0<ETP2/TP2≦3.
 14. The optical image capturing system of claim 10,wherein a thickness in parallel with the optical axis of the fifth lenselement at height ½ HEP is ETP5, a thickness of the fifth lens elementon the optical axis is TP5, and the following relation is satisfied:0<ETP5/TP5≦3.
 15. The optical image capturing system of claim 10,wherein a thickness in parallel with the optical axis of the sixth lenselement at height ½ HEP is ETP6, a thickness of the sixth lens elementon the optical axis is TP6, and the following relation is satisfied:0<ETP6/TP6≦5.
 16. The optical image capturing system of claim 10,wherein a distance from the first lens element to the second lenselement on the optical axis is IN12, and the following relation issatisfied: 0<IN12/f≦5.
 17. The optical image capturing system of claim10, wherein contrast transfer rates of modulation transfer with spatialfrequencies of 55 cycles/mm of an infrared wavelength 850 nm at theoptical axis on the image plane, 0.3 HOI and 0.7 HOI are respectivelydenoted by MTFI0, MTFI3 and MTFI7, and the following relations aresatisfied: MTFI0≧0.01, MTFI3≧0.01 and MTFI7≧0.01.
 18. The optical imagecapturing system of claim 10, wherein contrast transfer rates ofmodulation transfer with space frequencies of 110 cycles/mm of a visiblelight at the optical axis on the image plane, 0.3 HOI and 0.7 HOI arerespectively denoted by MTFQ0, MTFQ3 and MTFQ7, and the followingrelations are satisfied: MTFQ0≧0.2, MTFQ3≧0.01 and MTFQ7≧0.01.
 19. Theoptical image capturing system of claim 10, wherein at least one of thefirst, the second, the third, the fourth, the fifth and the sixth lenselements is a light filtration element with a wavelength less than 500nm.
 20. An optical image capturing system, from an object side to animage side, comprising: a first lens element with refractive power; asecond lens element with refractive power; a third lens element withrefractive power; a fourth lens element with refractive power; a fifthlens element with positive refractive power; a sixth lens element withnegative refractive power, and an image plane; wherein the optical imagecapturing system consists of six lens elements with refractive power, amaximum height for image formation on the image plane perpendicular tothe optical axis in the optical image capturing system is denoted byHOI, at least three lens elements among the first through sixth lenselements respectively have at least one inflection point on at least onesurface thereof, an object-side surface and an image-side surface of atleast one of the six lens elements are aspheric, focal lengths of thefirst through sixth lens elements are f1, f2, f3, f4, f5 and f6respectively, a focal length of the optical image capturing system is f,an entrance pupil diameter of the optical image capturing system is HEP,a half of maximum view angle of the optical image capturing system isHAF, a distance on an optical axis from an axial point on an object-sidesurface of the first lens element to an axial point on the image planeis HOS, a horizontal distance in parallel with the optical axis from acoordinate point on the object-side surface of the first lens element atheight ½ HEP to the image plane is ETL, a horizontal distance inparallel with the optical axis from a coordinate point on theobject-side surface of the first lens element at height ½ HEP to acoordinate point on the image-side surface of the sixth lens element atheight ½ HEP is EIN, and the following relations are satisfied:1.2≦f/HEP≦3.0, 0.4≦|tan(HAF)|≦3.0, HOI>3.0 mm and 0.2≦EIN/ETL<1.
 21. Theoptical image capturing system of claim 20, wherein a horizontaldistance in parallel with the optical axis from a coordinate point onthe image-side surface of the sixth lens element at height ½ HEP to theimage plane is EBL, a horizontal distance in parallel with the opticalaxis from an axial point on the image-side surface of the sixth lenselement to the image plane is BL, and the following relation issatisfied: 0.1≦EBL/BL≦1.1.
 22. The optical image capturing system ofclaim 21, wherein a horizontal distance in parallel with the opticalaxis from a coordinate point on the image-side surface of the fifth lenselement at height ½ HEP to a coordinate point on the object-side surfaceof the sixth lens element at height ½ HEP is ED56, a distance from thefifth lens element to the sixth lens element on the optical axis isIN56, and the following relation is satisfied: 0<ED56/IN56≦50.
 23. Theoptical image capturing system of claim 20, wherein a distance from thefifth lens element to the sixth lens element on the optical axis isIN56, and the following relation is satisfied: 0<IN56/f≦5.0.
 24. Theoptical image capturing system of claim 23, wherein the optical imagecapturing system satisfies the following relation: 0 mm<HOS≦30 mm. 25.The optical image capturing system of claim 23, further comprising anaperture stop, an image sensing device and a driving module, the imagesensing device is disposed on the image plane, a distance from theaperture stop to the image plane on the optical axis is InS, the drivingmodule and the six lens elements couple to each other and shifts areproduced for the six lens elements, and the following relation issatisfied: 0.5=InS/HOS≦1.1.